The proprietress of Ophelia's Kitchen is shocked to the core when the disciples put in a hurried order for food for 5000.
(Scene: Kitchen bench with cooking paraphernalia. Ophelia, the cook is busy mixing and singing to herself).
(To congregation) Oh hello there! Welcome to my little enterprise. I call it Ophelia's Kitchen. I'm Ophelia. Would you like a little supper prepared. Maybe a wedding feast. I can help you. Just the other week I catered for a wedding in Cana. Met some interesting people there, I can tell you! The Master was there too! I got to meet him, you know. He actually came out to my kitchen and … well that's another story.
Speaking of the Master, I got a note from him recently. He's ordered a special late night passover supper for 13. Funny thing is he doesn't need it until a year or so's time! Talk about forward planning! I wish some of my other customers were as organized! He made it quite clear that this meal is going to be too important to ignore. Humpf! I'd like to be a fly in the soup for that one!
Oh! Please don't worry. I run a tight ship here – it was just an expression. I'd die of shame if anyone suggested there were flies in the soups I make. That's probably why I'm so busy, up at the crack of dawn baking and mixing. It's not dull. I love it – but I do wish my husband would take a bit more interest in the business!
(Lightly) Ooh! Excuse me, another customer, just wait there, I'll talk to you in a moment.
Hello, Ophelia's Kitchen's. How may I help you? (pause, then conversationally) Peter! How are you, love? How's the Master? Yes. It is a busy life isn't it? (Pause) You want some catering done? O.K. just hold on pet, I'll get my book.
What? Urgent. TODAY! The Master wants to feed a hungry crowd. Yes! I know what that's like – you should see my family when they want to be fed – talk about crowds. My goodness! It certainly sounds like you've got a rowdy bunch there! (Laughs) Oh, you're such a tease Peter, 5000 indeed. No. No. Stop. Peter. Listen love, please - jokes aside. I need to know just exactly how many people I'm to cook for.
(Pause. A look of abject bewilderment). You can't be serious! You really do want me to cater for 5000 people - today?
I'm not sure I can help you, Peter love. You guys wouldn't have enough money to pay for a job this size, besides I just don't have the equipment, leave alone the ingredients. (Pause) Yes, I'll wait dear.
(To congregation - indignant) Would you believe that man! 5000 people today. Not even that scurrilous Greg the pie maker up the road could do it.
(Into phone) Hello – yes I'm here. That you again, Peter? (Pause, then laughs) Oh Peter, that's very sweet, but 3 fish and 5 loaves would barely feed my family of 4, even if I made fish soup! You can't possibly feed a crowd on that, but do thank the little boy for offering. Yes, Yes I'll wait (rolling eyes in frustration).
(To congregation) Just wait 'til I tell you this one. The Master wants me to cater for 5000 people on a hill in the middle of nowhere with a handful of fish and damper. If I could pull that one off – I'd make front page of the Galilee Times - probably win Caterer of the Year. Ah! If only!
(To phone) Oh, you're back! (listens) What is going on Peter! I can hardly hear you for the noise. What's happened?
(pause) They're all eating! WHAT? BUT HOW DID THE MASTER DO THAT? (flustered) IT'S IMPOSSIBLE – Stop joking me around Peter – it can't be true.
(pause) Matthew, oh Matthew tell me, is Peter telling me the truth? – He is! (pause then incredulous) TWELVE BASKETS! LEFTOVER? BUT THAT'S A MIRACLE!
(confused, shocked, bemused, breathless) Oh dear. Oh dear. Oh dear. Oh dear. Oh dear. Oh dear. (hangs up phone) Oh dear. Oh dear.
(To congregation) I'm sorry, I have to go. There are twelve baskets of leftover fish and damper that need my attention. (Gets up to go). You would never believe me in a million years!


Randall joined Trout, Ebersole & Groff, LLP in 2011. Prior to joining our firm, Randall was a finance manager at an international nonprofit organization, and a staff accountant at a public accounting firm. He currently serves on the firm's Manufacturing, Not-for-Profit, and Healthcare Practice Groups. He is also a member of the Multistate Taxation Committee.
As a Tax Department Manager, Randall handles all aspects of tax planning and preparation and business consulting for some of the firm's significant clients.
Randall enjoys activities with his family, playing various sports, volunteer work, and rooting for Philadelphia sports teams. He lives in Lancaster County with his wife and two children.


i found this adorable little note one morning last week.
little rikrak really cracks me up ... always.
inspired ... i'm gonna leave more cutiepie notes for dearies to find.
it's such a good feeling discovering them, isn't it?
found any cute notes around lately?
That's cute! My parents left each other sweet notes frequently when I was a child. I loved that idea, too. I should do it more!!!!!!
oh i love that story, moira!
oh that makes me teary just thinking about it, nicey! love love love that.
look what i won + look what YOU won!
the i love my sponsors MAY giveaway!
a fabulous giveaway with the little red door!
pull up a chair & read the modern sybarite!


text:
require "LuaScripts/Utilities/Sample"

local CTRL_FORWARD = 1
local CTRL_BACK = 2
local CTRL_LEFT = 4
local CTRL_RIGHT = 8

local CAMERA_DISTANCE = 10.0
local YAW_SENSITIVITY = 0.1
local ENGINE_POWER = 10.0
local DOWN_FORCE = 10.0
local MAX_WHEEL_ANGLE = 22.5

local vehicleNode = nil

function Start()
    -- Execute the common startup for samples
    SampleStart()

    -- Create static scene content
    CreateScene()

    -- Create the controllable vehicle
    CreateVehicle()

    -- Create the UI content
    CreateInstructions()

    -- Set the mouse mode to use in the sample
    SampleInitMouseMode(MM_RELATIVE)

    -- Subscribe to necessary events
    SubscribeToEvents()
end

function CreateScene()
    scene_ = Scene()

    -- Create scene subsystem components
    scene_:CreateComponent("Octree")
    scene_:CreateComponent("PhysicsWorld")

    -- Create camera and define viewport. Camera does not necessarily have to belong to the scene
    cameraNode = Node()
    local camera = cameraNode:CreateComponent("Camera")
    camera.farClip = 500.0

    renderer:SetViewport(0, Viewport:new(scene_, camera))

    -- Create static scene content. First create a zone for ambient lighting and fog control
    local zoneNode = scene_:CreateChild("Zone")
    local zone = zoneNode:CreateComponent("Zone")
    zone.ambientColor = Color(0.15, 0.15, 0.15)
    zone.fogColor = Color(0.5, 0.5, 0.7)
    zone.fogStart = 300.0
    zone.fogEnd = 500.0
    zone.boundingBox = BoundingBox(-2000.0, 2000.0)

    -- Create a directional light to the world. Enable cascaded shadows on it
    local lightNode = scene_:CreateChild("DirectionalLight")
    lightNode.direction = Vector3(0.3, -0.5, 0.425)
    local light = lightNode:CreateComponent("Light")
    light.lightType = LIGHT_DIRECTIONAL
    light.castShadows = true
    light.shadowBias = BiasParameters(0.00025, 0.5)
    light.shadowCascade = CascadeParameters(10.0, 50.0, 200.0, 0.0, 0.8)
    light.specularIntensity = 0.5

    -- Create heightmap terrain with collision
    local terrainNode = scene_:CreateChild("Terrain")
    terrainNode.position = Vector3(0.0, 0.0, 0.0)
    local terrain = terrainNode:CreateComponent("Terrain")
    terrain.patchSize = 64
    terrain.spacing = Vector3(2.0, 0.1, 2.0) -- Spacing between vertices and vertical resolution of the height map
    terrain.smoothing = true
    terrain.heightMap = cache:GetResource("Image", "Textures/HeightMap.png")
    terrain.material = cache:GetResource("Material", "Materials/Terrain.xml")
    -- The terrain consists of large triangles, which fits well for occlusion rendering, as a hill can occlude all
    -- terrain patches and other objects behind it
    terrain.occluder = true

    local body = terrainNode:CreateComponent("RigidBody")
    body.collisionLayer = 2 -- Use layer bitmask 2 for static geometry
    local shape = terrainNode:CreateComponent("CollisionShape")
    shape:SetTerrain()

    -- Create 1000 mushrooms in the terrain. Always face outward along the terrain normal
    local NUM_MUSHROOMS = 1000
    for i = 1, NUM_MUSHROOMS do
        local objectNode = scene_:CreateChild("Mushroom")
        local position = Vector3(Random(2000.0) - 1000.0, 0.0, Random(2000.0) - 1000.0)
        position.y = terrain:GetHeight(position) - 0.1
        objectNode.position = position
        -- Create a rotation quaternion from up vector to terrain normal
        objectNode.rotation = Quaternion(Vector3(0.0, 1.0, 0.0), terrain:GetNormal(position))
        objectNode:SetScale(3.0)
        local object = objectNode:CreateComponent("StaticModel")
        object.model = cache:GetResource("Model", "Models/Mushroom.mdl")
        object.material = cache:GetResource("Material", "Materials/Mushroom.xml")
        object.castShadows = true

        local body = objectNode:CreateComponent("RigidBody")
        body.collisionLayer = 2
        local shape = objectNode:CreateComponent("CollisionShape")
        shape:SetTriangleMesh(object.model, 0)
    end
end

function CreateVehicle()
    vehicleNode = scene_:CreateChild("Vehicle")
    vehicleNode.position = Vector3(0.0, 5.0, 0.0)

    -- Create the vehicle logic script object
    local vehicle = vehicleNode:CreateScriptObject("Vehicle")
    -- Create the rendering and physics components
    vehicle:Init()
end

function CreateInstructions()
    -- Construct new Text object, set string to display and font to use
    local instructionText = ui.root:CreateChild("Text")
    instructionText.text = "Use WASD keys to drive, mouse/touch to rotate camera\n"..
        "F5 to save scene, F7 to load"
    instructionText:SetFont(cache:GetResource("Font", "Fonts/Anonymous Pro.ttf"), 15)
    -- The text has multiple rows. Center them in relation to each other
    instructionText.textAlignment = HA_CENTER

    -- Position the text relative to the screen center
    instructionText.horizontalAlignment = HA_CENTER
    instructionText.verticalAlignment = VA_CENTER
    instructionText:SetPosition(0, ui.root.height / 4)
end

function SubscribeToEvents()
    -- Subscribe to Update event for setting the vehicle controls before physics simulation
    SubscribeToEvent("Update", "HandleUpdate")

    -- Subscribe to PostUpdate event for updating the camera position after physics simulation
    SubscribeToEvent("PostUpdate", "HandlePostUpdate")

    -- Unsubscribe the SceneUpdate event from base class as the camera node is being controlled in HandlePostUpdate() in this sample
    UnsubscribeFromEvent("SceneUpdate")
end

function HandleUpdate(eventType, eventData)
    if vehicleNode == nil then
        return
    end

    local vehicle = vehicleNode:GetScriptObject()
    if vehicle == nil then
        return
    end

    -- Get movement controls and assign them to the vehicle component. If UI has a focused element, clear controls
    if ui.focusElement == nil then
        vehicle.controls:Set(CTRL_FORWARD, input:GetKeyDown(KEY_W))
        vehicle.controls:Set(CTRL_BACK, input:GetKeyDown(KEY_S))
        vehicle.controls:Set(CTRL_LEFT, input:GetKeyDown(KEY_A))
        vehicle.controls:Set(CTRL_RIGHT, input:GetKeyDown(KEY_D))

        -- Add yaw & pitch from the mouse motion or touch input. Used only for the camera, does not affect motion
        if touchEnabled then
            for i=0, input.numTouches - 1 do
                local state = input:GetTouch(i)
                if not state.touchedElement then -- Touch on empty space
                    local camera = cameraNode:GetComponent("Camera")
                    if not camera then return end

                    vehicle.controls.yaw = vehicle.controls.yaw + TOUCH_SENSITIVITY * camera.fov / graphics.height * state.delta.x
                    vehicle.controls.pitch = vehicle.controls.pitch + TOUCH_SENSITIVITY * camera.fov / graphics.height * state.delta.y
                end
            end
        else
            vehicle.controls.yaw = vehicle.controls.yaw + input.mouseMoveX * YAW_SENSITIVITY
            vehicle.controls.pitch = vehicle.controls.pitch + input.mouseMoveY * YAW_SENSITIVITY
        end
        -- Limit pitch
        vehicle.controls.pitch = Clamp(vehicle.controls.pitch, 0.0, 80.0)

        -- Check for loading / saving the scene
        if input:GetKeyPress(KEY_F5) then
            scene_:SaveXML(fileSystem:GetProgramDir() .. "Data/Scenes/VehicleDemo.xml")
        end
        if input:GetKeyPress(KEY_F7) then
            scene_:LoadXML(fileSystem:GetProgramDir() .. "Data/Scenes/VehicleDemo.xml")
            -- After loading we have to reacquire the vehicle scene node, as it has been recreated
            -- Simply find by name as there's only one of them
            vehicleNode = scene_:GetChild("Vehicle", true)
            vehicleNode:GetScriptObject():PostInit()
        end
    else
        vehicle.controls:Set(CTRL_FORWARD + CTRL_BACK + CTRL_LEFT + CTRL_RIGHT, false)
    end
end

function HandlePostUpdate(eventType, eventData)
    if vehicleNode == nil then
        return
    end

    local vehicle = vehicleNode:GetScriptObject()
    if vehicle == nil then
        return
    end

    -- Physics update has completed. Position camera behind vehicle
    local dir = Quaternion(vehicleNode.rotation:YawAngle(), Vector3(0.0, 1.0, 0.0))
    dir = dir * Quaternion(vehicle.controls.yaw, Vector3(0.0, 1.0, 0.0))
    dir = dir * Quaternion(vehicle.controls.pitch, Vector3(1.0, 0.0, 0.0))

    local cameraTargetPos = vehicleNode.position - dir * Vector3(0.0, 0.0, CAMERA_DISTANCE)
    local cameraStartPos = vehicleNode.position
    -- Raycast camera against static objects (physics collision mask 2)
    -- and move it closer to the vehicle if something in between
    local cameraRay = Ray(cameraStartPos, (cameraTargetPos - cameraStartPos):Normalized())
    local cameraRayLength = (cameraTargetPos - cameraStartPos):Length();
    local physicsWorld = scene_:GetComponent("PhysicsWorld")
    local result = physicsWorld:RaycastSingle(cameraRay, cameraRayLength, 2)
    if result.body ~= nil then
        cameraTargetPos = cameraStartPos + cameraRay.direction * (result.distance - 0.5)
    end
    cameraNode.position = cameraTargetPos
    cameraNode.rotation = dir
end

-- Vehicle script object class
--
-- When saving, the node and component handles are automatically converted into nodeID or componentID attributes
-- and are acquired from the scene when loading. The steering member variable will likewise be saved automatically.
-- The Controls object can not be automatically saved, so handle it manually in the Load() and Save() methods

Vehicle = ScriptObject()

function Vehicle:Start()
    -- Current left/right steering amount (-1 to 1.)
    self.steering = 0.0
    -- Vehicle controls.
    self.controls = Controls()
end

function Vehicle:Load(deserializer)
    self.controls.yaw = deserializer:ReadFloat()
    self.controls.pitch = deserializer:ReadFloat()
end

function Vehicle:Save(serializer)
    serializer:WriteFloat(self.controls.yaw)
    serializer:WriteFloat(self.controls.pitch)
end

function Vehicle:Init()
    -- This function is called only from the main program when initially creating the vehicle, not on scene load
    local node = self.node
    local hullObject = node:CreateComponent("StaticModel")
    self.hullBody = node:CreateComponent("RigidBody")
    local hullShape = node:CreateComponent("CollisionShape")

    node.scale = Vector3(1.5, 1.0, 3.0)
    hullObject.model = cache:GetResource("Model", "Models/Box.mdl")
    hullObject.material = cache:GetResource("Material", "Materials/Stone.xml")
    hullObject.castShadows = true
    hullShape:SetBox(Vector3(1.0, 1.0, 1.0))

    self.hullBody.mass = 4.0
    self.hullBody.linearDamping = 0.2 -- Some air resistance
    self.hullBody.angularDamping = 0.5
    self.hullBody.collisionLayer = 1
    self.frontLeft = self:InitWheel("FrontLeft", Vector3(-0.6, -0.4, 0.3))
    self.frontRight = self:InitWheel("FrontRight", Vector3(0.6, -0.4, 0.3))
    self.rearLeft = self:InitWheel("RearLeft", Vector3(-0.6, -0.4, -0.3))
    self.rearRight = self:InitWheel("RearRight", Vector3(0.6, -0.4, -0.3))

    self:PostInit()
end

function Vehicle:PostInit()
    self.frontLeft = scene_:GetChild("FrontLeft")
    self.frontRight = scene_:GetChild("FrontRight")
    self.rearLeft = scene_:GetChild("RearLeft")
    self.rearRight = scene_:GetChild("RearRight")

    self.frontLeftAxis = self.frontLeft:GetComponent("Constraint")
    self.frontRightAxis = self.frontRight:GetComponent("Constraint")

    self.hullBody = self.node:GetComponent("RigidBody")

    self.frontLeftBody = self.frontLeft:GetComponent("RigidBody")
    self.frontRightBody = self.frontRight:GetComponent("RigidBody")
    self.rearLeftBody = self.rearLeft:GetComponent("RigidBody")
    self.rearRightBody = self.rearRight:GetComponent("RigidBody")
end

function Vehicle:InitWheel(name, offset)
    -- Note: do not parent the wheel to the hull scene node. Instead create it on the root level and let the physics
    -- constraint keep it together
    local wheelNode = scene_:CreateChild(name)
    local node = self.node
    wheelNode.position = node:LocalToWorld(offset)
    if offset.x >= 0.0 then
        wheelNode.rotation = node.worldRotation * Quaternion(0.0, 0.0, -90.0)
    else
        wheelNode.rotation = node.worldRotation * Quaternion(0.0, 0.0, 90.0)
    end
    wheelNode.scale = Vector3(0.8, 0.5, 0.8)

    local wheelObject = wheelNode:CreateComponent("StaticModel")
    local wheelBody = wheelNode:CreateComponent("RigidBody")
    local wheelShape = wheelNode:CreateComponent("CollisionShape")
    local wheelConstraint = wheelNode:CreateComponent("Constraint")

    wheelObject.model = cache:GetResource("Model", "Models/Cylinder.mdl")
    wheelObject.material = cache:GetResource("Material", "Materials/Stone.xml")
    wheelObject.castShadows = true
    wheelShape:SetSphere(1.0)
    wheelBody.friction = 1
    wheelBody.mass = 1
    wheelBody.linearDamping = 0.2 -- Some air resistance
    wheelBody.angularDamping = 0.75 -- Could also use rolling friction
    wheelBody.collisionLayer = 1
    wheelConstraint.constraintType = CONSTRAINT_HINGE
    wheelConstraint.otherBody = node:GetComponent("RigidBody")
    wheelConstraint.worldPosition = wheelNode.worldPosition -- Set constraint's both ends at wheel's location
    wheelConstraint.axis = Vector3(0.0, 1.0, 0.0) -- Wheel rotates around its local Y-axis

    if offset.x >= 0.0 then -- Wheel's hull axis points either left or right
        wheelConstraint.otherAxis = Vector3(1.0, 0.0, 0.0)
    else
        wheelConstraint.otherAxis = Vector3(-1.0, 0.0, 0.0)
    end

    wheelConstraint.lowLimit = Vector2(-180.0, 0.0) -- Let the wheel rotate freely around the axis
    wheelConstraint.highLimit = Vector2(180.0, 0.0)
    wheelConstraint.disableCollision = true -- Let the wheel intersect the vehicle hull

    return wheelNode
end

function Vehicle:FixedUpdate(timeStep)
    local newSteering = 0.0
    local accelerator = 0.0

    if self.controls:IsDown(CTRL_LEFT) then
        newSteering = -1.0
    end
    if self.controls:IsDown(CTRL_RIGHT) then
        newSteering = 1.0
    end
    if self.controls:IsDown(CTRL_FORWARD) then
        accelerator = 1.0
    end
    if self.controls:IsDown(CTRL_BACK) then
        accelerator = -0.5
    end

    -- When steering, wake up the wheel rigidbodies so that their orientation is updated
    if newSteering ~= 0.0 then
        self.frontLeftBody:Activate()
        self.frontRightBody:Activate()
        self.steering = self.steering * 0.95 + newSteering * 0.05
    else
        self.steering = self.steering * 0.8 + newSteering * 0.2
    end

    local steeringRot = Quaternion(0.0, self.steering * MAX_WHEEL_ANGLE, 0.0)
    self.frontLeftAxis.otherAxis = steeringRot * Vector3(-1.0, 0.0, 0.0)
    self.frontRightAxis.otherAxis = steeringRot * Vector3(1.0, 0.0, 0.0)

    if accelerator ~= 0.0 then
        -- Torques are applied in world space, so need to take the vehicle & wheel rotation into account
        local torqueVec = Vector3(ENGINE_POWER * accelerator, 0.0, 0.0)
        local node = self.node
        self.frontLeftBody:ApplyTorque(node.rotation * steeringRot * torqueVec)
        self.frontRightBody:ApplyTorque(node.rotation * steeringRot * torqueVec)
        self.rearLeftBody:ApplyTorque(node.rotation * torqueVec)
        self.rearRightBody:ApplyTorque(node.rotation * torqueVec)
    end

    -- Apply downforce proportional to velocity
    local localVelocity = self.hullBody.rotation:Inverse() * self.hullBody.linearVelocity
    self.hullBody:ApplyForce(self.hullBody.rotation * Vector3(0.0, -1.0, 0.0) * Abs(localVelocity.z) * DOWN_FORCE)
end

redpajama_set_name: RedPajamaGithub


text:
April 9th: Phonebank for Vote at Home during coronavirus
Apr 09 Apr 09, 2020 9:00am EDT - 9:00pm EDT Add to calendar 2020-04-09 09:00:00 2020-04-09 21:00:00 America/New_York April 9th, National Phonebank Day to make voting safe during coronavirus
The coronavirus pandemic is upending American life, and jeopardizing the 2020 primary and general elections. We can protect Americans and ensure our elections move forward as planned by ensuring voters in every state have vote at home options.

10 states do not allow voters to request absentee ballots, unless they have an excuse, and right now, the coronavirus does not qualify as an excuse. Governors have the power to change that, but only if they hear from the people.

Join our national phonebank to call voters in these 10 states and connect them with their Governors to demand vote at home options during the coronavirus crisis. Here's what you need to know:

When: Anytime between 9am and 9pm ET on April 9th

Where: Right from your computer!

Why: Keep voters safe through the coronavirus pandemic

Never phonebanked before? Don't worry - we'll train you on the script and dialer and make sure you have everything you need to start making calls.
 Ben Levinsohn [email protected]
The coronavirus pandemic is upending American life, and jeopardizing the 2020 primary and general elections. We can protect Americans and ensure our elections move forward as planned by ensuring voters in every state have vote at home options.
10 states do not allow voters to request absentee ballots, unless they have an excuse, and right now, the coronavirus does not qualify as an excuse. Governors have the power to change that, but only if they hear from the people.
Join our national phonebank to call voters in these 10 states and connect them with their Governors to demand vote at home options during the coronavirus crisis. Here's what you need to know:
When: Anytime between 9am and 9pm ET on April 9th
Why: Keep voters safe through the coronavirus pandemic
Never phonebanked before? Don't worry - we'll train you on the script and dialer and make sure you have everything you need to start making calls.
phonebank-auto phonebank-thanks
I'm bringing other people.

redpajama_set_name: RedPajamaCommonCrawl


Sunnyvale, CA and Newbury, UK (May 14, 2018): eGain (NASDAQ: EGAN), a leading provider of cloud-based customer engagement solutions, today announced the immediate availability of eGain® Solve™ for Amazon Connect.
Amazon Connect is based on the same contact center technology used by Amazon customer service associates around the world to power millions of customer conversations. The platform makes it easy for technology partners to integrate with its voice infrastructure, and businesses to deploy add-on solutions in a matter of minutes. Furthermore, the integration features comprehensive use of eGain's AI technology—from driving the IVR self-service dialog through call routing and guided help upon escalation to human-assisted service.
*Based on data from eGain clients.


text:
Q: Node.js-Express-Strompath No CustomData after immediately after registration I am having a strange error (at least in my opinion) after registering a user to stormpath via node/express using the Express-Stormpath module.
Just after registering I seem to have no access to customData in various routes for just the first user session. On registration I am creating and array for invoices
app.use(stormpath.init(app, {
    ...,
    expandCustomData: true,
    postRegistrationHandler: function(account, req, res, next) {

        account.customData.invoices = [];
        account.save();

        next();
    }
}));

but then when I go to access them in my index route I get this error
router.get('/', stormpath.loginRequired, function(req, res){

    console.log(req.user.customData.invoices ); // undefined

     res.render('index', {
        title: 'Index'
     });
});

how ever if I kill my local and restart it I get
 console.log(req.user.customData.invoices ); // []

which is what i would like.
Can anyone shed some light into what i am doing incorrectly here?
Thx in advance.

A: What's happening here is this: when you're inside of the postRegistrationHandler code -- customData won't be available automatically by default. The postRegistrationHandler is called immediately after registration before any of the helper functions have fun.
What you need to do to make your example work is first 'fetch' the customData from the Stormpath service.
Here's a working example:
app.use(stormpath.init(app, {
  ...,
  expandCustomData: true,
  postRegistrationHandler: function(account, req, res, next) {
    account.getCustomData(function(err, data) {
      if (err) return next(err);
      data.invoices = [];
      data.save();
      next();
    });
  }
}));

The above issue is really unclear in the docs -- this is 100% my fault (I'm the author of the library) -- I'll get this fixed today =)

redpajama_set_name: RedPajamaStackExchange


This ID represents the unique combination of a job, a credential, and a destination. The job log allows you to check usage, paper usage, operations and job history for each user or account.For details on viewing the output job logs, contact your service representative.On the See Oracle Database PL/SQL Packages and Types Reference for details on this type. Advanced Search Forum Technical Forums Copier Technical Discussion Sharp Job log error codes.
We were originally using scan to FTP and I switched the setting to scan to network folder but I'm still receiving these errors. share|improve this answer edited Aug 12 '10 at 11:42 answered Aug 11 '10 at 20:27 Riccardo Murri 9,3563133 1 Case 3: The script didn't produce any output, therefore no email If, however, the job creator turns on full logging and the class-specific level is set to record runs only, the higher logging level of the job takes precedence and all operations Thanks in advance!
So, if you don't get any output, there are basically three possibilities: crond could not even start a shell for running the program or sending email crond had troubles mailing the BEGIN DBMS_SCHEDULER.REMOVE_JOB_EMAIL_NOTIFICATION ( job_name => 'EOD_JOB', recipients => '[email protected], [email protected]', events => 'JOB_DISABLED, JOB_SCH_LIM_REACHED'); END; / When you specify multiple recipients and multiple events, the notification for each specified event is This example accepts the defaults for the sender, subject, and body arguments. This feature is not available for OpenVMS and will be ignored if specified.
You can also provide a filter condition, and only job state events that match the filter condition generate notifications. To enable multiple state change event types in one call, you add the desired bit flag values together and supply the result as an argument to SET_ATTRIBUTE. Retain for: This field indicates whether you want the centrally managed log file(s) to be retained for a specified period of time. For a scan to HDD job, the number of stored black & white pages is recorded. 13 Full Color Total Count For a print job, the total count is recorded.
This queue is a secure queue, so depending on your application, you may have to configure the queue to enable certain users to perform operations on it. Ask Your Own Printers Question Customer: replied2 years ago. If you want to keep that behaviour you should look into tee(1). Your applications subscribe to this queue, dequeue event messages, and take appropriate actions.
Poker Chip Alternative Take a ride on the Reading, If you pass Go, collect $200 Does flooring the throttle while traveling at lower speeds increase fuel consumption? I will add the link for the error codes to my docs for future reference. 0 Anaheim OP Helpful Post edgarcastellanos Dec 15, 2015 at 10:12 UTC Hi For example, you can configure a job to send an e-mail to both the principle DBA and one of the senior DBAs whenever the job fails with error code 600 or Expert: Russell H.
The following example shows job log entries for a complete job lifecycle. All other arguments have defaults. You can view the log file(s) from the Job History tab as well as determine where the files are located. Indicates the minimum severity level that causes a message to be returned to a user or program.
mailx(1) is the basic mail reading program on most every Unixlike system. Submitted: 2 years ago. It may not be a good solution if your cronjob generates hundreds of lines of output. For a send job, the number of transmitted black & white pages is recorded.
is very unlikely, but something should have been written in the cron logs. Reply With Quote 01-29-2015 #3 ICWILL View Profile View Forum Posts Private Message Junior Member Join Date Jan 2015 Location La Crosse Posts 2 Post Thanks / Like Thanks (Given) 2 The message could indicate that a function is in progress or that it has reached a successful completion. 10 - Warning: A message of this severity indicates a potential error condition. Results 1 to 5 of 5 Thread: Job log error codes.
See Also: "Monitoring and Managing Window and Job Logs" for more information about setting the job class logging level Monitoring Multiple Destination Jobs For multiple-destination jobs, the overall parent job state A doc feeder jam while faxing or scanning would cause this. 80 is a NIC connect failure. When you specify multiple recipients and multiple events, each recipient is notified when any of the specified events is raised. That's of interest.
MX-M623N » Bookmarks Bookmarks Digg del.icio.us StumbleUpon Google Posting Permissions You may not post new threads You may not post replies You may not post attachments You may not edit your A routing step may have ended abnormally or failed to start, a job-level function may not have been performed as required, or the job may have been ended. 60 - System It describes a condition that renders either a subsystem or the whole system inoperative. 99 - Action: A message of this severity indicates that some manual action is required, such as Archive after retention period..: By default, when a log file's retention period expires the file is deleted.
Centrally managed log files means that ActiveBatch will handle the complete specification of the log and/or error files and the directories they are created in. In case 2., you should inspect the mailer daemon logs: messages from the Cron daemon usually appear as from [email protected] See attached bulletin for explanation of errors Attached Files Explanation of Error Cause Codes in the Job Log.pdf (298.7 KB, 171 views) Reply With Quote 01-29-2015 #5 ICWILL View Profile View Expert: Russell H.


text:
Name: KINGFORM HEALTH HOMETEXTILE GROUP LIMITED (KFG)
Date of Listing: 08 June 2012
Date of Delisting: 07 September 2017
This entity was delisted from the Australian Securities Exchange on 07 September 2017.
KINGFORM HEALTH HOMETEXTILE GROUP LIMITED (KFG)
2012 ALL
Our website ranking of KFG:
KFG website
KFG email
KFG investorRelations
KFG announcements
KFG directors
Link Market Services, Rhodes Corporate Park, 1A Homebush Bay Drive, Rhodes NSW 2138
Tel : +61 1300 554 474
Address: UNIT 101 15 BOND STREET CAULFIELD NORTH VIC 3161
Company Secretary: Xun Yang
Sector: Consumer Durables & Apparel
Industry Group: XDJ
Activities: Design, development, manufacturing and distribution of household textile products
delisted from the close of trading on Thursday, 07 September 2017 pursuant to Listing rule 17.12.
we understand the company has been delisted because of failure to have its securities quoted for more than three years
The company releases a letter to its shareholders. The matters set out in the schedule previously released will be attended to on or before the dates referred to in the announcement.
The company lodges its Preliminary Final Report 2017.
The company lodges its Half Yearly Report ending 31 December 2016.
The company lodges its 2016 Annual Report to shareholders.
The company releases its Appendix 4G.
The company lodges an updated Half Yearly Report ending 31 December 2015.
The company outlines its business plans for the next 12 - 18 months.
The financial and sales figures before 30 June 2017 are coming soon. At this time, the company has confirmed sales contracts worth AUD $1.64 million for the export of products which are to be shipped within 3 months after 1 July 2017.
ShineWing Australia has been appointed as auditor of the company effective 22 August 2017. This appointment follows the resignation of BDO Audit (WA) Pty Ltd, and ASIC's consent to the resignation.
In the first half of 2017, the company's amount of sales reached more than RMB 22.27 million, a 45% increase over the same period last year.
The company made some upgrading in its equipment in the first half of 2017 due to the increase in orders for production in sales.
The company details its current operation and activities in Australia. The Company mainly sells all kinds of household textiles to retailers and distributors in Australia, which are both necessities and every-day consumptions, with great market potential. The Company's management goal in Australia is to let China's products and services into Australia, Australian products sold into China, to maximize the investors benefit and to contribute to the Australia economy.
The company has been advised to demonstrate to ASX its compliance with listing rule 12.1 and all other listing rule compliance from listing to date. The company then advises in relation to the activities of KFG and addresses that the company has much activitiy and operations to comply with the requirements.
The company releases the chairman's letter to shareholders regarding the AGM on 25 August 2017. The meeting will be held at 15 Bond Street, Caulfield North, Victoria, 3161, Australia. The meeting will begin at 1:30 (Australian Eastern Standard Time or AEST) with registration available from 1:00pm (AEST).
The company issues a Response to ASX Query.
The following entity (Kingform Health Hometextile Group Limited) has not paid their annual listing fees in respect of the year ending 30 June 2016 but the securities are already suspended from official quotation. Under listing rule 17.15, any entity that has not paid its annual listing fees as required by listing rule 16.5 by 5.00 pm AEST on Monday 31 August 2015 will be removed from the official list with effect from the close of trading on Monday 31 August 2015
The company releases the proxy form for the AGM
The company gives notice that its Annual General Meeting will be held on Friday, 17 July 2015 in Suite 2, Level 8, 303 Collins Street, Melbourne, Australia. The Meeting will begin at 10:30am (AEST) with registration from 9:30am (AEST).
The securities of Kingform Health Hometextile Group Limited will be suspended from official quotation from the commencement of trading today 1 September 2014 following the failure to lodge its Preliminary Final Report for the period ending 30 June 2014 in accordance with Listing rules.
The suspension of trading in the securities of Kingform Health Hometextile Group Limited will be lifted before the commencement of trading tomorrow, following lodgement of the half yearly accounts for the period ended 31 December 2013. Security Code: KFG
The securities of Kingform Health Hometextile Group Limited will be suspended from official quotation from the commencement of trading today 3 March 2014 following failure to lodge its periodic reports for the period ended 31 December 2013 in accordance with listing rules.
The securities of Kingform Health Hometextile Group Limited will be suspended from Official Quotation from the commencement of trading today 1 March 2013 following failure to lodge its Half Year Report and/or Accounts for the period ended 31 December 2012 in accordance with Listing rules.
The suspension of trading in the securities of Kingform Health Hometextile Group Limited will be lifted before the commencement of trading tomorrow, following lodgement of the annual report for the period ended 30 June 2012. Security Code: KFG
securities suspended following failure to lodge full year accounts to 30 June 2012
KINGFORM HEALTH HOMETEXTILE GROUP LIMITED
Chen Li CFO
Yang Xun Independent Director 08/06/2012
Paul Nolan Independent Director 08/06/2012
Xiaofei Wei Non Exec Director 20/07/2017
Jin Xikang Executive Director, CEO 08/06/2012


My favorite part about this vegan meatball sliders appetizer is that they can be made ahead of time and assembled right before you need them.
Following up from yesterday's post on my vegan cocktail party menu, I am excited to share my meatball slider recipe with you today.
My favorite part about this appetizer is that they can be made ahead of time and assembled right before you need them. If you want a make-ahead option, make and bake the balls, then freeze. To heat up, warm spaghetti sauce in either a saucepan or crock pot and add the meatballs. Once thawed and warmed through, add to the slider buns! For the party, I choose the crockpot option for an easy serve option and to keep the stove free of clutter.
Add the onion a pinch of salt, and saute until translucent. Add the garlic, red pepper flakes, dried oregano and basil. Stir together and cook another 2-3 minutes.
Add the mushrooms, reduce the heat to medium-low and cook until mushrooms are reduced and browned.
Stir in the red wine and deglaze, scrapping up any browned bits at the bottom of the pan. Continue to cook until the liquid has evaporated.
Add the mixture to a food processor bowl along with the beans, carrots, and sun-dried tomatoes. Pulse until mixture comes together.
Add the breadcrumbs, nutritional yeast, parsley, and pinch salt/pepper. Pulse to combine. You don't want a puree, but it should stick together with relative ease.
Place in a bowl and let chill in the refrigerator for 1/2 hour.
Roll into balls, for the sliders, they should be big enough to place onto a slider bun. If you are making this for another use, you can make the meatballs as large/small as you desire.
Cooking step 1, saute: Heat 1 tbsp. olive oil in a saute pan and add the formed balls. Cook over medium-high heat for about one minute on each side. You want the balls to get slightly crunchy/browned on the outside.
Cooking step 2, Add the browned balls to a lightly sprayed or parchment lined baking sheet and cook at 375 degrees F for 20 minutes.
Warm the marinara sauce in a saucepan & add the meatballs.
Place a meatball and 1 tbsp. spaghetti sauce on each slider bun.
That sounds and looks so amazing…after trying vegan (cashew) cheez which used Natural Mesquite (H20, natural mesquite smoke flavor, vinegar, molasses, caramel color). That might be a good addition to make them smoky, grilled or BBQ'd. Just a thought…will put this on the recipe list to try…TU for sharing.
Great ideal Millie! I am actually planning on using a similar meatball for BBQ meatballs this weekend for another party! I will have to try that cheese!


text:
\section{Introduction}\label{sect:intro}

The Gross~-~Neveu (GN) model,  originally introduced in~\cite{Gross:1974jv} in 1974 as a toy model for a study of
dynamical symmetry breaking,  found its application in many areas of physics. The model describes a system of
fermion fields with a quartic interaction. It is renormalizable in two dimensions, asymptotically free and, moreover, admits
an exact solution~\cite{Zamolodchikov:1978xm}. Above two dimensions the $N$-component GN~-~model is renormalizable within the
$1/N$ expansion technique. It possesses a nontrivial  Wilson~-~Fisher
fixed point and gives an example of a conformal field theory (CFT) in $d$-dimensions. Basic critical indices of the GN model
are available at
$1/N^2$ order~\cite{Gracey:1990wi,Gracey:1992cp,Derkachov:1993uw,Vasiliev:1993pi,Gracey:1993kb}
 and the index $\eta$~--~the
anomalous dimension of the fermion field~--~at $1/N^3$~\cite{Vasiliev:1992wr,Gracey:1993kc}. These results were obtained by
methods of the self-consistency equation  and conformal bootstrap  developed
in~\cite{Vasiliev:1981yc,Vasiliev:1981dg,Vasiliev:1982dc}.
A recent revival of interest to this model is due to a relevance of fermionic systems with quartic interactions to the
description of the phase transition in graphene \cite{Janssen:2016xvc}.

The UV completion  of the GN model contains an additional scalar field  with  a quartic self-interaction and is known as the
Gross-Neveu-Yukawa (GNY) model \cite{ZinnJustin:1991yn}.  Moreover, the chiral extension of the GNY model -- the
Nambu-Jona-Lasinio (NJL) model -- describes, for a low number of fermion flavors,   a system with an emergent
supersymmetry~\cite{Fei:2016sgs}.
The recent calculation of the corresponding  renormalization group (RG) functions
with four-loop accuracy ~\cite{Karkkainen:1993ef,Mihaila:2017ble,Zerf:2017zqi}  confirms the emergence of supersymmetry at the
critical point.

The four--loop calculations are quite involved and carried out with the help of computer algebra. The results available from
$1/N$ expansion provide an additional check for the perturbative calculations. The  four loop RG
functions obtained in~\cite{Zerf:2017zqi} are in a perfect agreement with the results of $1/N$
calculations~\cite{Gracey:1990wi,Gracey:1992cp,Derkachov:1993uw,Vasiliev:1993pi,Gracey:1993kb,Vasiliev:1992wr,Gracey:1993kc}.
In this paper we present $1/N^2$ expressions for the other two indices -- the so-called correction exponents that are related to
the slopes of
$\beta$ functions at the critical point and were known only with $1/N$ accuracy ~\cite{Gracey:2017fzu}.

The $1/N$ calculations are usually done with the help of the methods of the self-consistency equations or conformal bootstrap
\cite{Vasiliev:1981yc,Vasiliev:1981dg,Vasiliev:1982dc}. These methods are very effective for the calculation
of the critical indices of the basic and auxiliary fields, but are not very suitable in the case of local operators.
Therefore we use a different method developed
in~\cite{Vasiliev:1975mq,Vasiliev:1993ux,Derkachov:1997ch}. A detailed description of the method can be found
in~\cite{Derkachov:1997ch,Derkachov:1998js} and an application to the GN model in~\cite{Manashov:2016uam}.

The paper is organized as follows: In sect.~\ref{GNY} we recall the formulation of the GNY model and show that the slopes of
$\beta$ functions at the critical point coincide with the critical dimensions of  certain operators of dimension four.
In sect.~\ref{largeN} we review briefly the  $1/N$ expansion technique for the GN model and present the rules for calculating
the anomalous dimensions of local operators. Section~\ref{diagrams} contains the details of the calculation of the correction
exponents at order~$1/N^2$.  In \ref{app:1/n^2indices} we  collect expressions for relevant basic indices. \ref{app:SEV}
contains details of the calculation of the self-energy and vertex correction diagrams and in \ref{app:part_results} we collect
results for the individual diagrams.

\section{Gross-Neveu-Yukawa model in $d=4-2\epsilon$ dimensions}\label{GNY}
The Lagrangian of the GNY model in $d=4-2\epsilon$ Euclidean space takes the form
\begin{align}
\mathcal{L}=
\frac12(\partial\sigma)^2+\bar q\slashed{\partial} q+g_1 \sigma \bar q q+ g_2\sigma^4,
\end{align}
where $q$ is the $N$-component fermion field and $\sigma$ is a scalar field.
 The model is multiplicatively renormalized~\cite{ZinnJustin:1991yn}
\begin{align}\label{eq:ren_action}
 \mathcal{L}_R = \frac{Z_1}2(\partial\sigma)^2 +Z_2\bar q\slashed{\partial}q
+M^\epsilon Z_3 g_1 \sigma \bar q  q
+M^{2\epsilon}Z_4 g_2\sigma^4.
\end{align}
Here $M$ is the renormalization scale and $Z_i$ are the renormalization constants. In MS-like schemes the renormalization
factors $Z_i$ are given by a series in
$1/\epsilon$,
$Z_i=1+\sum_k z_{i}^k/\epsilon^k$.

The anomalous dimensions of the fields and the $\beta$ functions are defined as usual
\begin{align}
  \gamma_q =\mathcal{ D}_M \ln Z_q, &&
  \gamma_\sigma = \mathcal{D}_M \ln Z_\sigma, &&\beta_i=\mathcal{ D}_M g_i,
\end{align}
where  $Z_\sigma= Z_1^{1/2}$ and $Z_q = Z_2^{1/2}$ and
\begin{align}\label{DM}
\mathcal{D}_M \equiv M\frac{d}{dM}=M\partial_M+\beta_1\partial_{g_1}+\beta_2\partial_{g_2}\,.
\end{align}
The GNY model  possesses non-trivial  fixed points
\begin{align}
  \beta_1(g_1^\ast,g_2^\ast) = 0 , &&
  \beta_2(g_1^\ast,g_2^\ast) = 0.
\end{align}
One of this points is infrared stable, i.e. the eigenvalues of the matrix
\begin{align}
\omega_{ik}=\partial_i \beta_k\big|_{g=g^\ast}
\end{align}
are both positive. These eigenvalues, $\omega_\pm$,
are called correction indices. The indices $\omega_\pm$ can be identified with the anomalous dimensions of certain composite
operators that will be discussed in the rest of this section.

The partition function $Z(J)$ defined by the path integral
\begin{align}\label{ZJ}
Z(J)=\int D\bar q Dq D\sigma \exp\left\{-S_R+ \int d^dx\,\, J(x)\,\Phi(x)\right\},
\end{align}
where $J=\{j,\eta,\bar \eta\}$ and $J\Phi=j\sigma+\bar\eta q+\bar q\eta$,  is  finite in perturbation theory. Moreover,
derivatives of \eqref{ZJ} with respect to the renormalized couplings $g_i$  are finite, too. Thus one concludes that
\begin{align}
\partial_{g_k} \mathcal{L}_R= \sum_a c_a [\mathcal{O}_a]+ \partial \mathcal{ B}\,,
\end{align}
where the sum goes over some set of renormalized operators of the canonical dimension four with finite coefficients~$c_a$. By
$\partial \mathcal{ B}$ we denote terms (not necessarily finite) which vanish after integration. Since
\begin{align}
\partial_{g_1} \mathcal{L}_R \equiv M^{\epsilon} \sigma \bar q q + \text{singular $1/\epsilon$ terms}
\end{align}
and similar for another derivative one concludes that
\begin{align} \label{eq:der_action_ren}
\partial_{g_1}\mathcal{L}_R & = M^{\epsilon} [\sigma \bar q q]\equiv M^\epsilon[\mathcal{O}_1] ,
\notag\\
\partial_{g_2} \mathcal{L}_R &= M^{2\epsilon} [\sigma^4]\equiv M^{2\epsilon} [\mathcal{O}_2],
\end{align}
where we omitted terms with total derivatives.

Applying the operator~\eqref{DM}  to both sides of Eqs. \eqref{eq:der_action_ren} and taking into account that
$\mathcal{D}_M S_R=\mathcal{D}_M S_0=0$ one derives the RG equation for the operators $[\mathcal{O}_k]$
\begin{align} \label{eq:RGE}
\Big(\delta_{ik}\mathcal{D}_M  +\gamma_{ik}\Big)[\mathcal{O}_k] =0\,,
\end{align}
where the anomalous dimension matrix $\gamma$ has the following form
\begin{align}\label{eq:gammacrit}
  \gamma =
  \begin{pmatrix}
    \epsilon + \partial_{g_1} \beta_{1} & M^{\epsilon} \partial_{g_1} \beta_{2} \\
     M^{-\epsilon} \partial_{g_2} \beta_{1} & 2\epsilon + \partial_{g_2} \beta_2
  \end{pmatrix}.
\end{align}
Using the known lowest order expression for  the beta-functions (see e.g. ref.~\cite{Zerf:2017zqi}) one finds that at the
Wilson-Fisher critical point  the anomalous dimensions take the form
\begin{align}
\gamma =
  \begin{pmatrix}
    3\epsilon & 0 \\
    0 & 4\epsilon
  \end{pmatrix} +O(1/N).
\end{align}
resulting in the following  scaling dimensions for  the operators $\mathcal{O}_\pm$,
\begin{align}
\Delta & =\Delta_\text{can}+\gamma_\ast
\notag\\
& = d+\begin{pmatrix}
    \partial_{g_1} \beta_{1} & M^{\epsilon} \partial_{g_1} \beta_{2} \\
     M^{-\epsilon} \partial_{g_2} \beta_{1} &  \partial_{g_2} \beta_2
  \end{pmatrix}=4+O(1/N).
\end{align}
Diagonalizing the matrix $\Delta$ one constructs two operators whose scaling dimensions are given  by the eigenvalues
of~$\Delta$. Scaling dimensions of  operators are physical observables and do not depend on a regularization, expansion,
subtraction scheme, etc. We use this property to calculate the anomalous dimension of the operators $[\mathcal{O}_\pm]$  in
$1/N$ expansion.

\section{Large $N$ expansion for the GN model}\label{largeN}
The GNY model is critically equivalent to the  $d$-dimensional $N$-component GN model, i.e.  critical indices in both models
coincide. In the GN model the indices can be calculated using the $1/N$ expansion. Below we briefly review the method that we
use for the calculation. A more extensive review of the $1/N$ techniques including the self-consistency equations and conformal
bootstrap can be found in the book~\cite{Vasilev:2004yr}.

Let us write the action of the GN model in the form suitable for generating
the $1/N$ expansion
\begin{align}\label{N-GN}
S_{GN} &=\int d^d x\left[\bar q\slashed{\partial} q+\sigma \bar q q -\frac{N}{2g} \sigma^2\right]\,.
\end{align}
Here $q=\{q^i, i=1,\ldots,N\}$ is the $N$-component fermion field and $\sigma$ is an auxiliary scalar field which can be
excluded by the equation of motion (EOM). At a certain (critical) value of the coupling, $g=g_*$ the system undergoes a second order phase
transition. At  this point correlators of the basic and auxiliary fields
$q,\bar q, \sigma$ exhibit  power law behaviour and, as it can be shown, the model enjoys  scale and conformal
invariance~\cite{Derkachov:1993uw}.

It can be shown that in the {\it infrared region} (IR) the dominant contribution to the propagator of the $\sigma$-field comes
from the fermion loop~\cite{ZinnJustin:1991yn}
\begin{align}\label{sigma-prop}
D_\sigma(x)=-\frac1n {B(\mu)}/{x^2}\,.
\end{align}
Here $n=N\,\text{tr} \II$, where the trace is taken in the space of $d$-dimensional spinors
 and the normalization factor is
\begin{align}\label{bmu}

B(\mu)=\frac{4\Gamma(2\mu-1)}{\Gamma^2(\mu)\Gamma(\mu-1)\Gamma(1-\mu)}\,.
\end{align}
For practical calculations   it is convenient to use  a simplified (massless) version of the GN model which is critically
equivalent to~\eqref{N-GN}. The action of the model is given by the following expression~\cite{Vasiliev:1975mq,Vasilev:2004yr}
\begin{align}\label{L-GN}
S'_\Delta &=\int d^d x\left[\bar q\slashed{\partial} q -\frac12 \sigma L_\Delta\sigma +\sigma \bar q q  + \frac12 \sigma L\sigma\right]\,.
\end{align}
The kernel $L$
has the form
\begin{align}
L(x) & = \mathrm{tr} D_q(x) D_{q}(-x)
=-n
{A^2(\mu)}/{x^{2(2\mu-1)}}\,,
\end{align}
where $D_q$ is the fermion propagator
\begin{align}
D_q(x) =-
\frac{A(\mu)\slashed{x}}{x^{2\mu}} \,, &&A(\mu)=\frac{\Gamma(\mu)}{2\pi^\mu}\,.
\end{align}
The regularized kernel $L_\Delta$ is
\begin{align}\label{Ldef}
L_\Delta(x)= L(x) (M^2 x^2)^{-\Delta} C^{-1}(\Delta)\sim x^{-2(2\mu-1+\Delta)}\,.
\end{align}

The first two terms in~\eqref{L-GN} can be viewed as the free part of the action, $S_0$, and the remaining ones -- as an
interaction.
The last term in~\eqref{L-GN} cancels diagrams with insertions of simple fermion loops in the
$\sigma$-lines. As a consequence, in the leading order the propagator of the $\sigma$ field
is given by the inverse kernel $L_\Delta$. It this work we fix the constant $C(\Delta)$, which is arbitrary save the condition
$C(0)=1$, by the requirement for the propagator $D_\sigma$ to have the following form
\begin{align}
D_\sigma(x)=-  \frac1{n} B(\mu)(M^{2}x^2)^\Delta/{x^2}\,.
\end{align}
The parameter $\Delta$ should be considered as a regularization parameter. The divergences in the correlators appear as
poles in $\Delta$ and are removed by adding the counterterms to the action~\eqref{L-GN}. The renormalized action takes the form
\begin{align}\label{L-GN-ren}
S'_{R} &=\int d^d x\left[Z_1\bar q\slashed{\partial} q -\frac12 \sigma L_\Delta\sigma + Z_2 \sigma \bar q q
+ \frac12 \sigma L\sigma\right]\,.
\end{align}
Though the model is renormalizable, the renormalization is not multiplicative, i.e.  $S'_R(q,\sigma) \neq S'(q_0,\sigma_0)$.
Due to the non-multiplicative character  of the renormalization  the anomalous dimensions of the fields and operators cannot
be, in general, determined via the corresponding renormalization factors. However, as it was shown in~\cite{Derkachov:1997ch}
this problem appears  starting from
$1/n^3$ order only. Up to the order $1/n^2$ the anomalous dimension of the operators can be obtained via the renormalization
factors as follows. First, one has to modify the $\sigma$-propagator by multiplying it by some parameter $u$,
$D_\sigma \mapsto u D_\sigma$ and determine the renormalization factors calculating  the corresponding diagrams with the modified propagator.
Let $\mathcal{O}_i$ be a system of operators mixing under renormalization,
\begin{align}
[\mathcal{O}_i(\Phi)] =(\mathbf{Z}(u))_{ik} \mathcal{O}^B_k(\Phi_0)\,,
&&
 \mathbf{Z}(u)=1+\sum_{a=1}^\infty \frac{Z_a(u)}{\Delta^a}\,,
\end{align}
where $\Phi=\{q,\bar q, \sigma\}$, and $\mathcal{O}^B_i$ are bare operators. Up to the order $1/n^2$ the anomalous
dimensions for the operators can be obtained as follows~\cite{Derkachov:1997ch}
\begin{align}\label{gamma-O}
\gamma_{ik}= 2\partial_u (\mathbf{Z}_1(u))_{ik}\Big|_{u=1} +O(1/n^3)\,.
\end{align}
We use this formula for the calculation of the anomalous dimensions of the operators in question.

\section{Correction exponents at $1/n^2$}\label{diagrams}
\begin{figure}[t]
  \centering
  \includegraphics[width=0.5\columnwidth]{Mixing}
  \caption{The $1/n^2$ diagram $\sigma^3\mapsto \sigma\partial^2\sigma$ which could contribute to the element $\gamma_{21}$ of the mixing
  matrix. }
  \label{fig:Mixing}
\end{figure}
In the perturbative expansion the correction exponents to the scaling are related to the scaling dimensions of the operators
$\sigma^4$ and
$\sigma \bar q q$. The scaling dimensions of these operators are $\Delta_a=4+O(1/n)$. Let us first identify the corresponding
operators in the $1/n$ expansion. There exist three scalar operators of dimension four,
$$
\mathcal{O}=\{\sigma^4,\sigma\partial^2\sigma,  \partial^2 \sigma^2\}.
$$
\begin{figure*}[t]
\begin{minipage}{\linewidth}
\centering
  \includegraphics[width=0.52\linewidth]{g3A}\\[3mm]
  \includegraphics[width=0.99\linewidth]{Bseries}
  \caption{Feynman diagrams $D_{1}- D_3$ (first line) and $D_4- D_7$ (second line)
contributing to the anomalous dimensions $\Delta \gamma_{\sigma^3}$ }
  \label{fig:Dgamma3}
  \end{minipage}
\end{figure*}
 The last one is a total derivative and can be
neglected. Note here that the operator $\sigma\bar q q$ in the $1/n$ expansion has the dimension $4-2\epsilon+O(1/n)$.
Therefore it does not mix with the above operators and has no relation to the correction exponents~\footnote{The universality
hypothesis states that theories in the same universality class possess the same spectrum of  scaling dimensions, but the
corresponding operators can have  different implementation.}. Thus we need to find the anomalous dimension matrix for the
operators
$\mathcal{O}_+=\sigma^4$ and $\mathcal{O}_-={\sigma\partial^2\sigma}$.

It is easy to see that
 the diagonal entries $\gamma_{11}$, $\gamma_{22}$ and $\gamma_{12}$ of the anomalous dimension matrix are of order $1/n$. At the same time the anomalous
 dimension $\gamma_{21}$ is of order $1/n^3$. It happens because the only diagram which contributes  to this matrix element at order
 $1/n^2$, $\sigma^3\mapsto \sigma\partial^2\sigma$, see Fig.~\ref{fig:Mixing},
does not diverge. It can be checked by an explicit calculation.
 Also, the finiteness of this diagram is guaranteed by the conformal symmetry. The arguments are exactly the same as in the case of
 $\sigma^2\mapsto \partial^2\sigma$ transition in the nonlinear $\sigma$ model. An interested reader can find detailed
 discussions in  Refs.~\cite{Derkachov:1997gc,Derkachov:1998js}. Thus at the order $1/n^2$ one can neglect mixing and
 calculate only the diagonal matrix elements.

We will use either upper or lower index for  the coefficients  of the $1/n$ expansion
\begin{align}
\gamma=\sum_{k=0}^\infty \gamma_k/n^k=
\sum_{k=0}^\infty \gamma^{(k)}/n^k
\end{align}
  trying  to keep  notations close to   generally
accepted. For the reader's convenience we collect $1/n^2$ expressions
for the basic indices ($\eta=2\gamma_q$,
$\gamma_\sigma=-\eta-\kappa$ and $\lambda=(d-\Delta[\sigma^2])/2$) in \ref{app:1/n^2indices}.

\subsection{Operator $\sigma^\ell$}

Here we present our result for the anomalous dimension of the operator $\sigma^\ell$. The mixing  affects the anomalous
dimension of this operator only starting from $1/n^3$. Analyzing  the contributing diagrams  it is easy to notice that
the anomalous dimension for the operator
$\sigma^\ell$ can be written in the form
\begin{align}
\gamma_{\sigma^\ell}=-\ell(\ell-2)\gamma_\sigma+
C^\ell_2\gamma_{\sigma^2} +
C^\ell_3\Delta\gamma_{\sigma^3}+O(1/n^3)\,,
\end{align}
where $C^\ell_k$ are the binomial coefficients. The anomalous dimension $\gamma_\sigma$ and $\gamma_{\sigma^2}$ are known with
$1/n^2$ accuracy~\cite{Gracey:1992cp,Gracey:1990wi,Derkachov:1993uw,Vasiliev:1993pi}, see \ref{app:1/n^2indices}. The last
contribution starts from $1/n^2$. The diagrams contributing to
$\Delta\gamma_{\sigma^3}$ are shown in Fig. \ref{fig:Dgamma3}.
Their calculation  is rather straightforward so we will not dwell on it. We obtained  the following expression for
$\Delta\gamma_{\sigma^3}$
\begin{align}
  \Delta \gamma_{\sigma^3}^{(2)} =
\eta_1^{2}\frac{6\mu^2}{\mu-1}\Big[&-\frac{(3\mu-2)(2\mu-1)}{\mu-1}\notag
\\
&+(3\mu-1)\big[\psi'(\mu)-\psi'(1)\big]
\Big]\,.
\end{align}
Here $\psi(x)$ is the Euler $\psi$ function and an explicit expression for the index $\eta_1=-B(\mu)/2\mu$ can be found in
\ref{app:1/n^2indices}.  Thus for the correction index $\omega_+$ we find
\begin{align}\label{eq:omega+}
\omega_+&=2\Big(\epsilon-4\gamma_\sigma + 3\gamma_{\sigma^3}+2\Delta \gamma_{\sigma^3}+O(1/n^3)\Big)
\notag\\
&=2\epsilon +\frac{\eta_1}{n}\frac{4(2\mu-1)(3\mu-1)}{\mu-1}+\ldots
\end{align}
The explicit expression for the $1/n^2$ correction, $\omega_+^{(2)}$, is rather lengthy and will not be given here. Instead we
present an expansion of the index $\omega_+$
around $\mu =2-\epsilon$ up to  $\epsilon^4$ terms
\begin{align}
\omega_+^{(0)}&=2\epsilon\,,
\notag\\
\omega_+^{(1)}&= 120\epsilon-212\epsilon^2-26\epsilon^3 +\big(-29+240 \zeta_3\big)\epsilon^4\,,
\notag\\
\omega_+^{(2)}&=-5040\epsilon+7380\epsilon^2 + 2\big(8767+6624\zeta_3\big)\epsilon^3
\notag\\
&\quad +
32\left(-392 + 621 \zeta_4 - 2226\zeta_3 - 420\zeta_5\right)\epsilon^4\,,
\end{align}
in complete agreement with the results of the four--loop calculation~\cite{Zerf:2017zqi}.

\subsection{Operator $\sigma\partial^2\sigma$}
In this section we discuss diagrams contributing to the anomalous dimension of  the operator $\mathcal O_-= \sigma
\partial^2\sigma$ which, as usual, can be split in two parts
\begin{align}
\gamma_-=\widehat \gamma +2\gamma_\sigma\,.
\end{align}
In the leading order in $1/n$ only the two diagrams shown in Fig.~\ref{fig:g-LO} contribute to
$\widehat \gamma$.
\begin{figure}[H]
  \centering
  \includegraphics[width=0.7\linewidth]{g-LO}
  \caption{ The LO diagrams contributing
to the anomalous dimension~$\gamma_{-}$. The circled cross denotes
an operator insertion $\mathcal O_-$. }
  \label{fig:g-LO}
\end{figure}
\noindent The first diagram has the symmetry coefficient $C_{\text{sym}}=2$. The calculation of both diagrams is rather
straightforward and leads to the following expression
\begin{gather}
\widehat \gamma_1 =   2 \eta_1
{(4 \alpha^2- 1)}/{\alpha},
\end{gather}
where we introduced the notation $\alpha \equiv \mu-1$. Taking into account that $\gamma_\sigma^{(1)}=-\eta_1(1+\mu/\alpha)$
one obtains for
$\gamma_-$
\begin{align}
\gamma_-^{(1)}=\eta_1 \frac{4(2\mu-1)(\mu-2)}{\mu-1}
\end{align}
that agrees  with the result of~\cite{Gracey:2017fzu} derived with the help of the  self-consistency equations approach.

At the  order $1/n^2$  there are in total $23$ different diagrams to be calculated. Namely,
\begin{itemize}
\item
    $4$ operator vertex correction diagrams, Fig.~\ref{fig:OC}
\ite
    $12$ self-energy insertion and vertex correction diagram
\ite
    $3$~single box diagrams, Fig.~\ref{fig:SingleBox}
\ite
    $4$ double box diagrams, Fig. \ref{fig:DoubleBoxes}
\end{itemize}
Before presenting our final answer for $\widehat \gamma$ we briefly discuss the calculation of the diagrams.
\begin{figure}[H]
  \centering
  \includegraphics[width=\columnwidth]{OC}
  \caption{ Operator vertex correction diagrams.
}
  \label{fig:OC}
\end{figure}
\begin{itemize}
\item In order to calculate the operator correction diagrams it is sufficient to calculate
the $1/n$ order diagrams up to
    finite,
$O(\Delta^0)$, terms.  For the sum of the two diagrams we obtained~\footnote{We do not display  factors like
$t^\Delta=e^{-\Delta \psi(1)+\ldots}$ which drop out from the final answer.}
 $\mathbb D (\Delta)= u^2
 D(\Delta)/\Delta$, where

\begin{align}
 D(\Delta) &=-\frac{\widehat \gamma_1}{4
\Biggl\{
1-\Delta\biggl[2B_3 -\frac{3\mu(\mu-1)(\mu-2)}{(2\mu-1)(2\mu-3)} C_1
\notag \\
&\quad
+ \frac{\mu^5-9\mu^4+21\mu^3-9\mu^2-6\mu+4}{(2\mu-1)\mu(\mu-1)(\mu-2)}
\biggr]
\Biggr\}\,,
\end{align}
where  we accepted the notations of~\cite{Vasilev:2004yr}
\begin{align}
B(x) &=\psi(x)+\psi(x')\,, &&
C_x=\psi'(x)-\psi'(x'),
\end{align}
$ B_k=B(k-\mu)-B(1)$ and $x'\equiv \mu-x$.

The answer for the operator correction diagrams ($D_\text{OC}) $ reads
\begin{align}
KR'(D_\text{OC}) &= u^4\left(
\frac{D(\Delta)}{\Delta}\frac{ D(2\Delta)}{2\Delta}-
\frac{D(0)D(\Delta)}{\Delta^2}\right)
\notag\\
&=\frac12 u^4 D^2(0)\left(-\frac1{\Delta^2}+\frac1{\Delta} \frac{D'(0)}{D(0)}\right)\,.
\end{align}
\item Instead of calculating separately  each diagram of the second group, that is not quite simple, we use the result
    of~\cite{Derkachov:1997ch} where it was shown that the contribution of all such diagrams to the anomalous dimension can
    be extracted from the $1/n$ order diagrams with dressed propagators and vertices. We   discuss  details of the
    calculation in \ref{app:SEV} .

\item The single box diagrams shown in Fig.~\ref{fig:SingleBox} as well as double box diagrams, Fig. \ref{fig:DoubleBoxes},
    have only a superficial divergence.
\begin{figure}[H]
  \centering
  \includegraphics[width=0.98\columnwidth]{Cseries}
  \caption{ Single box diagrams $SB_1$ - $SB_3$.
}
  \label{fig:SingleBox}
\end{figure}
\vskip -5mm After integration over the operator insertion coordinate one gets a propagator  type diagram,

    \begin{align}
    D_k(x)= A_k(\Delta)/x^{2(\mu+1-3\Delta)}\,.
    \end{align}

The $\Delta$ pole arises after the Fourier transform. For the anomalous dimension it is sufficient to know $A_k(\Delta)$ at
$\Delta=0$. Since in coordinate space the diagram is finite at $\Delta\mapsto 0$, one can put $\Delta=0$ from the beginning.
It greatly simplifies  calculations since one can use the star~-~triangle relation for the basic  $\sigma \bar q q$ vertex,
shown in Fig.~\ref{fig:star-triangle}.
\begin{figure}[H]
  \centering
  \includegraphics[width=0.92\columnwidth]{star-triangle}
  \caption{ The star-triangle relation. The indices $\alpha,\beta,\gamma$ satisfy the uniqueness condition
  $\alpha+\beta+\gamma=2\mu-1$, $a(x)=\Gamma(x')/\Gamma(x)$ and $x'=\mu-x$.
}
  \label{fig:star-triangle}
\end{figure}
 Next, multiplication by $x^2$ makes the diagrams logarithmically divergent, i.e. the residue of the $\Delta$ pole does not
depend on the external momenta. Thus one can use the freedom to change the momentum flow through a diagram to facilitate
calculations~\cite{Vladimirov:1979zm}. For example, to calculate the second  diagram in Fig.~\ref{fig:SingleBox} it is
convenient to choose the momentum flow (after a multiplication by $x^2$) through the vertices connected to the crossed
circle (operator insertion) and use the star-triangle relation for the upper $\sigma \bar q q$ vertex. After this
transformation the diagram is calculated by consecutive application of chain integration rules.

\item The calculation of the first three double box diagrams which follows the same pattern is more involved and one has to
    use many tricks like the integration by part~\cite{Chetyrkin:1981qh}, the tetrahedron
    transformation~\cite{Gorishnii:1984te}, etc. A review of the relevant multiloop calculation techniques can be found
    in~\cite{Vasilev:2004yr}. \vskip-2mm
\begin{figure}[H]
  \centering
  \includegraphics[width=0.98\columnwidth]{DoubleBoxes}
  \caption{ Double box diagrams $DB_1$ (top left) - $DB_4$ (bottom right).
}
  \label{fig:DoubleBoxes}
\end{figure}
\vskip -3mm In principle the last double box diagram could be calculated in the same way. However it is more convenient
 to apply an inversion transformation first, simplify the numerators and use the star-triangle relation for
the bosonic triangle. As the result one gets
a sum of three- and two-loop diagrams whose calculation is more or less straightforward.

\end{itemize}

Finally, collecting contributions from  all diagrams (see ~\ref{app:part_results}) we obtain for
$\widehat\gamma_2$
 {\allowdisplaybreaks
\begin{align}
 \widehat \gamma_2 = &
\eta_1 \Biggl\{
-\frac{8 (2 \alpha -1) \left(2 \alpha ^3+5 \alpha -2\right)}{(\alpha -2) (\alpha -1) \alpha} \notag
\\
  &+\eta_1\biggl(

  {3 \left(4 \alpha ^3+2 \alpha ^2+1 -1/\alpha\right)
  C_
 \notag \\
  &+\left[32 \alpha ^2+\frac{2}{\alpha ^2}+40 \alpha +\frac{36}{\alpha -2}+\frac{20}{\alpha
   -1}-\frac{6}{\alpha }+40\right]B_3 \notag \\
  &+8 \alpha ^3+\frac{4}{\alpha ^3}-8 \alpha ^2-\frac{12}{\alpha ^2}-14 \alpha
   -\frac{18}{\alpha -2}\notag \\
&+\frac{72}{\alpha -1}-\frac{18}{\alpha +1}+\frac{20}{(\alpha-1)^2}+\frac{10}{\alpha }+84
  \biggr)
\Biggr\}.
\end{align}}
 Thus for the second correction exponent we get

 \begin{align}
 \omega_-  =2\epsilon+\gamma_- +O(1/n^3)=2\epsilon +2\gamma_\sigma+\widehat\gamma+ O(1/n^3)\,.
 \end{align}

Substituting the expressions for $\gamma_\sigma$ and $\widehat\gamma$ and expanding around $\mu=2-\epsilon$ up to $\epsilon^4$
terms one obtains
\begin{align}
\omega_-^{(0)} =&2\epsilon\,,
\notag\\
\omega_-^{(1)} =&-24 \epsilon ^2+28 \epsilon ^3+22 \epsilon ^4\,,
\notag\\
\omega_-^{(2)} =& 174 \epsilon ^2+\left(432 \zeta_3-293\right)\epsilon ^3   \notag \\
&-2\left(1500 \zeta_3-324 \zeta_4+419\right)  \epsilon ^4\,,
\end{align}
that agrees with the results of \cite{Zerf:2017zqi}.

\section{Summary}\label{summary}
We have calculated the correction exponents $\omega_\pm$ in the GN model with $1/n^2$ accuracy. These exponents are related to
the slopes of the beta functions in the critical GNY model. Our results are in complete agreement with the expressions for the
perturbative  four loop beta functions in the GNY model obtained recently in~\cite{Zerf:2017zqi}. For the calculation we used
the method developed in~\cite{Vasiliev:1975mq,Vasiliev:1993ux,Derkachov:1997ch}. This method allows one to use the standard RG
technique and, at the same time, to resum effectively a certain subset of diagrams reducing the total number of diagrams to be
calculated. Values for each individual diagram are presented in~\ref{app:part_results} and will be useful for
calculations of the corresponding exponents  in  the chiral versions of the GN model.

\begin{acknowledgements}
This work was supported by Deutsche Forschungsgemeinschaft (DFG) with the grants
$\text{MO~1801/1-2}$ (A.M.) and SFB/TRR 55 (M.S.)
\end{acknowledgements}

redpajama_set_name: RedPajamaArXiv


European and US regulators have signed an agreement allowing them to share commercially confidential information, include trade secrets, relating to medicine inspections.
The European Commission, the FDA and the European Medicines Agency said the confidentiality agreement is a milestone in a programme to mutually recognise inspections of manufacturers.
The new agreement is certain to cut paperwork by allowing the two regulators to use each other's good manufacturing practice inspections of drug manufacturing plants.
It is the culmination of nearly three years of co-operation between the FDA and EU and will allow the two regulators to rely on information from drug inspections conducted within each other's borders.
This will cut duplication of inspections, lower costs, and enable the regulators to devote more resources to other parts of the world where there may be greater risk.
In 2012, the US congress passed legislation allowing the FDA to make agreements to recognise drug inspections by foreign regulators it considers capable of conducting inspections that meet US standards.
This led to a collaboration between the FDA and EU in 2014 to evaluate the way they each carry out inspections, and assessing the risks and benefits of mutual recognition of drug inspections.
The EU and US already had confidentiality agreement in place since 2003, allowing them to exchange confidential information as part of their regulatory and scientific process, but complete exchange of information was not possible under these arrangements.
Scott Gottlieb, the FDA's commissioner, gave his backing to the agreement on Twitter.
From a UK perspective, this major step forward in collaboration underlines the risks of Brexit. By leaving the EU, the UK is likely to miss out on the benefits of greater alignment, and will inevitably not be in the vanguard of this process.


text:
/*
panel.css (part of editor.css)
================================

Panels are floating elements that can hold different types of contents.
The following are common uses of it:

	- The element that toolbar combos display when opening them.
	- The context menu.
	- The list of items displayed by "menu buttons" (e.g. scayt).
	- The panel shown when opening "panel buttons" (e.g. color buttons).

Panel contents are wrapped into an iframe, so it is possible to have additional
CSS loaded inside them (e.g. to have more accurate preview on the styles combo).

The following is a visual representation of the outer elements of a panel:

+-- .cke_panel(*) ---------------------+
| +-- IFRAME.cke_panel_frame --------+ |
| | +-- HTML.cke_panel_container --+ | |
| | | +-- .cke_panel_block ------+ | | |
| | | |                          | | | |
| | | |     (contents here)      | | | |
| | | |                          | | | |
| | | +--------------------------+ | | |
| | +------------------------------+ | |
| +----------------------------------+ |
+--------------------------------------+

(*) All kinds of panel share the above structure. Menu panels adds the
    .cke_menu_panel class to the outer element, while toolbar combos add the
	.cke_combopanel class.

This file also defines styles for panel lists (used by combos). For menu-like
panel contents and color panels check menu.css and colorpanel.css.
*/

/* The box that holds an IFRAME. It's inserted into a host document and positioned
   absolutely by the application. It floats above the host document/editor. */
.cke_panel
{
	/* Restore the loading hide */
	visibility: visible;
    width: 120px;
   	height: 100px;
   	overflow: hidden;

	background-color: #fff;
    border: 1px solid #d1d1d1;
}

/* This class represents panels which are used as context menus. */
.cke_menu_panel
{
	padding: 0;
	margin: 0;
}

/* This class represents panels which are used by rich combos. */
.cke_combopanel
{
    width: 150px;
    height: 170px;
}

/* The IFRAME the panel is wrapped into. */
.cke_panel_frame
{
	width: 100%;
	height: 100%;
	font-size: 12px;

	overflow: auto;
	overflow-x: hidden;
}

/* The HTML document which is a direct descendant of the IFRAME */
.cke_panel_container
{
	overflow-y: auto;
	overflow-x: hidden;
}

/* Remove focus outline. The .cke_panel_block gets focused after combo without any active item is selected. */
.cke_panel_block:focus
{
	outline: none;
}

/*
Here we start the definition of panel lists (e.g. combo panels). The following
is its visual representation:

+-- .cke_panel_block -----------------+
| +-- .cke_panel_grouptitle --------+ |
| |                                 | |
| +---------------------------------+ |
| +-- .cke_panel_list --------------+ |
| | +-- .cke_panel_listItem ------+ | |
| | | +-- a --------------------+ | | |
| | | | +-- span -------------+ | | | |
| | | | |                     | | | | |
| | | | +---------------------+ | | | |
| | | +-------------------------+ | | |
| | +-----------------------------+ | |
| | +-- .cke_panel_listItem ------+ | |
| | | +-- a --------------------+ | | |
| | | | +-- span -------------+ | | | |
| | | | |                     | | | | |
| | | | +---------------------+ | | | |
| | | +-------------------------+ | | |
| | +-----------------------------+ | |
| | ...                             | |
| +---------------------------------+ |
+-------------------------------------+
*/

/* The list of panel items. */
.cke_panel_list
{
	margin: 0;
	padding: 0;
	list-style-type: none;
	white-space: nowrap;
}

/* The item of .cke_panel_list */
.cke_panel_listItem
{
	margin: 0;
	padding: 0;
}

/* The child of .cke_panel_listItem. These elements contain spans which are
   to display a real name of the property which is visible for an end-user. */
.cke_panel_listItem a
{
	padding: 6px 7px;
	display: block;
	color: inherit !important;
	text-decoration: none;
	overflow: hidden;
	text-overflow: ellipsis;
}

.cke_hc .cke_panel_listItem a
{
	border-style: none;
}

.cke_panel_listItem.cke_selected a,
.cke_panel_listItem a:hover,
.cke_panel_listItem a:focus,
.cke_panel_listItem a:active
{
	background-color: #e9e9e9;
}

/* Redefine focus outline so it is the same for all browsers. */
.cke_panel_listItem a:focus
{
	outline: 1px dotted #000;
}

.cke_hc .cke_panel_listItem a:hover,
.cke_hc .cke_panel_listItem a:focus,
.cke_hc .cke_panel_listItem a:active
{
	border: 2px solid;
	padding: 4px 5px;
}

/* The following styles set defaults of the elements used by the Paragraph
   Format panel. */
.cke_panel_listItem p,
.cke_panel_listItem h1,
.cke_panel_listItem h2,
.cke_panel_listItem h3,
.cke_panel_listItem h4,
.cke_panel_listItem h5,
.cke_panel_listItem h6,
.cke_panel_listItem pre
{
	margin-top: 0px;
	margin-bottom: 0px;
}

/* The title of the entire panel which is visible on top of the list. */
.cke_panel_grouptitle
{
	cursor: default;
	font-size: 11px;
	font-weight: bold;
	white-space: nowrap;
	margin: 0;
	padding: 6px 6px 7px 6px;

	color: #484848;
	border-bottom: 1px solid #d1d1d1;
	background: #f8f8f8;
}


High School Honors: Two-year Baseball letter winner; pitcher on two PIL Championship Teams; pitcher on State Championship American Legion Team. Hockey letter winner; member of Championship Teams.
Post High School Career: Signed professional contract at age 17; Played for Hollywood Stars of Pacific Coast League and Cincinnati Reds and St. Louis Cardinals in the National League.


text:
80± Acres
Harper County, Kansas
Contact Brochure (620) 388-6328 Text Me Maps
Ask Nathan Leeper
80+/- Acres of Great Hunting and Pasture in Harper County, Kansas.
Acres: 80±
Type: Farms, Hunting Land, Ranches
City, State: Attica, Kansas
County: Harper
Lat/Long: 37.19457, -98.25045
Presented By: Nathan Leeper
Email: Click to Contact
Legal Description: N/2 of the NW/4 of S12-T33s-R9w.
Driving Directions: Take Main Street south out of Attica, Kansas and head approximately 3 miles. Turn west on NW 30th rd and go 1/2 mile. The farm is on the south side of the road.
2021 Taxes: $185.18
Property Description: You will be hard pressed to find a better turn key 80 in South Central, Kansas. Located in deer Unit 16 just 1 hour from Wichita, and 20 minutes from Anthony and Harper Kansas. This Harper County farm has a lot to offer for a new land owner wanting to get started hunting, building a new home, or even running a cattle operation. The seller has done many upgrades to this farm. It has new hedge post 5 wire fence on 2 sides, with new steal gates and rocked entrances on the north and west sides. It has a new water well with a timer ( needs repair ). It also has a 2 year old insulated 10x12 Tuff Shed with a loft and a work bench, perfect for a night stay and a place to store tools. Power is supplied on the west side of the property and offers 220 and 110 outlets with a LED security light over looking the parking area and shed. The expired CRP grass and multiple mulberry trees provide excellent cover for big mature Kansas bucks, pheasant, quail, and predators. DO NOT over look this farm as it sits on its own island of cover surrounded by tillable acres. The deer love to stay in this thick cover and get away from other pressured areas. The east end of the property has a spring fed creek that has thick cedar trees growing along it. The middle part of the farm has a nice pond that rarely goes dry. On the cattle side of things this is a very affordable 80 that hasn't been grazed in many years. With new fence and no lack of water it will make a great buy before this years grazing season. With power and water on the property you could build your dream home not far off a black top road. The water well and electric is right along the road on the west side of the property.
What mineral rights are owned by the Sellers shall transfer. It is believed to be 50%. There are no active lease on the property. CRP is expired. 1 old water well on the property.
For more information or to schedule a showing contact Nathan Leeper at 620-388-6328.
Secluded Cover
Spring Fed Creek
New Fence
Great Deer, Pheasant, Quail, and Predator Hunting
Expired CRP
Cattle Pasture
Great Trail Camera History
SW of Attica Kansas 3.5 Miles
20 Minutes From Harper / Anthony
1 Hour From Wichita Airport (ICT)
Nathan Leeper
Preston, Kansas
Ask Nathan About This Property


text:
Q: docker command is showing nothing in centos7 hi i just installed latest version of docker in Virtual machine with Cent OS 7 and yum update finished.
but my docker's command doesn't work,showing nothing,even docker is on the service list.
and what if i type in service docker status the active menu displaying active(running" since ****")
it was same as such as tried remove and install again.
please check image file what i attached.
thanks
I took screen shot my problem and what i tried


text:
August 1990 sees the launch of 1st new national radio station for 20 years - radio 5 - which will carry sport, education and world service broadcasts. OU programmes will have a new slot.
Penny Vine
Susan Rae
Unit 1 Objectives
Objectives for S100 Unit 01
Icons - Entertainers
The fourth in the ICONS series, Entertainers is an hour-long documentary charting t...he story of Entertainment in the 20th Century. Tonight's episode sees Hollywood star Kathleen Turner examine the achievements and legacies of four of the Century's greatest entertainers. The story of Entertainment in the 20th Century ranged from vaudeville clowns to Space Oddities, and everything in between. This was 100 years where technological developments changed the face of entertainment forever – givin
The managers : episode 4 - German football legend Jurgen Klinsmann
This summer Jurgen Klinsmann will take the USA team to the World Cup final. He will... be trying to become just the third person to win the trophy as a player and as a manager. The odds are stacked against him; the USA team he took over in 2011 are one of the outsiders for the trophy.But, there is no doubt that Jurgen Klinsmann is one of the most insightful and interesting managers in world football, and in the run up to the start of the tournament Peter Bowes meets him in Los Angeles, where he has
Enterprise in Education: OU scheme for students to further careers - new pack avail...able in May 1991. OBS tour England to launch new professional certificate.


Ken Jeong (The Hangover) and David Hasselhoff (Baywatch) star in the most hilarious and outrageous comedy of the year. When a struggling nightclub owner (Jeong) fails to pay back a loan shark, he decides the only way to get the money is to kill his pick in the annual "Who Will Die This Year" celebrity death pool: David Hasselhoff. But the task is not so easy – especially when your target is The Hoff.


text:
How IoT can help cities survive the holiday 'shipmageddon'
The sooner delivery services begin tapping available technologies, the sooner we can reduce chronic issues like holiday congestion and shipping delays.
By Jonathan Sparks
Editor's Note: The following is a guest post from Jonathan Sparks, VP of IoT products at ServiceNow.
COVID-19 is disrupting so many facets of our lives, including the way we will celebrate this holiday season. Online shopping, which has consistently grown over the last several years, has surged during the pandemic and promises to peak at over $189 billion in online holiday spend this year.
Experts have forecast a "shipmageddon" this winter, with extreme delays as already overburdened shipping companies struggle to keep pace with rising demand — and cities may acutely feel the impact. As delivery trucks crisscross main streets, double park on busy streets to offload packages and create mazes of gridlock, traffic could come to a grinding halt.
Emerging technologies like IoT-enabled devices and artificial intelligence (AI) will play a critical role in helping transportation companies avoid extreme delays, for both holiday gifts and drivers. By harnessing these technologies, packages can get out on time and cities can make certain that congestion does not rise to extreme levels, ensuring that the holiday season remains the most wonderful time of the year.
Getting packages on their way faster
For logistics companies, the holiday season is already the equivalent of the Super Bowl. With the projected exponential rise in online shopping this year, the spotlight on these companies will get brighter — and there will be less room for failure.
As inventory comes and goes at all hours of the night, IoT-enabled pallets will provide managers with a single view of the warehouse and offer increased opportunities for organization and optimization of deliveries. Using AI, spacing can optimize the placement of packages for distribution, removing the need for workers to zig-zag across the warehouse to get packages into trucks.
When packages are closely monitored and directed with AI on a single platform, all teams involved in shipping have visibility into the same streamlined data, and managers can keep their focus on sending out trucks at a steady and regulated pace. This consistent rhythm keeps distribution normal and ensures that cities aren't overburdened with too many trucks at the same time.
By combining the power of IoT and AI, logistics companies can further streamline the distribution of packages. Something that will be critical given the incredible volume of boxes, containers and parcels that will be entrusted to them for safe and timely deliveries.
Of course, shipping companies can only control so much. Cities have a role to play in combating the "shipmageddon" as well.
Keeping traffic rolling and curbs clean
Managing traffic in major metropolitan areas has long been a struggle, and anyone who has driven in a large city can personally attest to the opportunities for improvement. It should be of no surprise, then, that many cities – from Columbus, OH to Austin, TX to Los Angeles – are already turning to technology to address congestion. The impending rise of holiday deliveries will put these systems to the test.
Many of the devices used to help mitigate traffic jams and keep vehicles flowing through cities leverage remote controlled devices like changeable speed limit signs, radar, stop lights and road signs. All of them will need to work overtime this holiday season to endure wave after wave of delivery trucks. However, if everything is not working in harmony, streets can quickly become mired in gridlock with trucks needing to drop off deliveries on already crowded streets.
A single location to control all these critical systems and provides a comprehensive street-to-street view is essential for keeping pace with rising traffic problems.
By incorporating IoT and AI across traffic devices, cities can ensure that changes made to reduce traffic levels are reflected everywhere. If an IoT-connected road sign tells drivers to divert to a particular street due to construction, AI can alert the stop light on that street to change its timing to accommodate for the increased number of cars and allow for more packages to get to their destination on time.
Cities can also utilize IoT to ensure that these tools are in working order. A stoplight going down in the middle of the day can back up a city for hours – the kind of a backup during peak delivery hours that can envelop an entire neighborhood.
With information such as location and time of the stoplight failure, in a single platform, city officials can keep track of all devices on the network and use early detection to fix an issue before it devolves into a traffic nightmare and schedule maintenance during off-hours to reduce congestion. With IoT monitoring, device downtime is reduced, and, in some cases, issues are resolved even before drivers are aware of a problem.
The future of deliveries is now
Even when all these systems work in harmony, there will still be traffic and delays can happen. IoT-equipped devices can detect backups before they begin, and AI can push out an alert to inform drivers. Cities that utilize IoT technology can quickly share traffic data with delivery companies to alert dispatchers to hot spots and reroute trucks accordingly to avoid layering on to backups. Likewise, delivery companies can alert customers to updated timelines based on traffic data, keeping them informed with the latest.
Though the surge in online shopping is unavoidable this year, the "shipmageddon" scenario can be prevented. Delivery companies and cities need to leverage technology like IoT and AI to ensure a smooth holiday delivery season as well as a reliable and streamlined process all year round.
By deploying these technologies now, everyone wins. The city of the future will be digitally connected, and the sooner that services like delivery begin tapping into that vision, the sooner we can start to reduce chronic issues like holiday congestion and shipping delays.
Filed Under: Transportation Tech & Data
davidpheat. Retrieved from https://pixabay.com/photos/cityscape-city-road-crossroad-1186069/.
11 experts predict what will shape smart cities in 2021
From electrification to digital twins and the "15-minute city," respondents shared a wide variety of trends to watch in the new year.
By Kristin Musulin, Cailin Crowe and Chris Teale • Dec. 15, 2020
In a time when connection is more important than ever, cities are tapping innovative tools and strategies to engage their citizens and keep communities healthy.
Retrieved from Flickr user Kim Seng on November 13, 2020
5G health concerns sow uncertainty amid ongoing rollout
While deployment continues unabated across the U.S., a small coalition of groups and leaders are trying to put the brakes on 5G in a bid to learn more about the technology.


Abstract: The effect of harvesting method on fruit quality and storability of the pink-fleshed 'Foster' grapefruits, at 18±1°C and 85%-90% r.h., was evaluated. The traditional method, using a hooked pole, was compared with an improved technique, where the picking pole was equipped with a long cloth sleeve held open by a ring for collecting the harvested fruits. The fruits were stored for three months at 18±1°C and 85%-90% r.h. Fruit samples were taken at specific times for determination of fruit quality in terms of respiration rate, total soluble solids (TSS), water loss and titratable acidity. At the termination of the experiment, the fruits were evaluated for general quality. The results showed that the improved method significantly decreased respiration rate and water loss, delayed TSS accumulation and reduced titratable acidity, resulting in improved fruit quality, reduced post-harvest losses and extended shelf-life of fruits.


Not a big token state. Not a lot of tokens or collectors. However, rare Connecticut tokens, Connecticut saloon, and Connecticut good for mirror's can be found. If you are new to Connecticut tokens check out the pieces for sale below.
Connecticut Tercentenary 1635-1935 The Charter Oak BEAUTIFUL!!
Celluloid Starch Co. Token New Haven Connecticut Good For One Celluloid Package!


Spoken word artist Nego True returns to our ears with another powerful piece of artistry, in the form of 'Letter To My Little Sister'. A deep emotion lead track, raw with memories and strong in love.
Although this is a very personal piece of poetry, it conveys a message that many siblings can relate to, displaying a touching sequence of words that can sometimes be very difficult to find, and even tougher to express.
This entry was posted in New Releases, Spoken Word, Videos and tagged Artist, Letter To My Little Sister, London, Lost In The Sound, Nego True, Poet, Spoken Word, UK. Bookmark the permalink.


On Sunday, February 18, IRONMAN celebrated the 40th anniversary of its very first triathlon event, which took place in Oahu, Hawai`i in 1978, and with-it kick-off the IRONMAN 40 Years of Dreams campaign. Throughout the course of the 2018 IRONMAN and IRONMAN 70.3 event series, the campaign will be rolled out in a variety of ways, leading up to the IRONMAN World Championship in Kailua-Kona, Hawai`i on October 13.
To follow the IRONMAN 40 Years of Dreams celebration all year long, visit Ironman.com/40yearsofdreams.
As you plan your 2018 season, who better to consult than your fellow athletes? Our annual athlete surveys tell the story best: using the information we gather from YOU, our community, we are proud to present our top 10 IRONMAN and IRONMAN 70.3 events across a variety of categories. Read on for the places and communities that will get you excited to race this year—whether you're looking for a pristine swim, a memorable post-race party, or a bike course that will leave you drooling.
The drama was in the women's race where Switzerland's Nina Derron seemed to have the race in control as she demolished the field on the bike to take a 6:13 lead on to the run. Melbourne rookie Grace Thek who has a U.S. college running background, began to eat into the lead, down to 2:42 at halfway and 1:19 back with 7kms left. She took the lead with 3kms remaining but Derron kept in touch. When Thek fell once on the chute, got up and ran on, but fell again almost within reach of the line, the Swiss athlete edged past for the win while Aussie Laura Dennis completed the podium, three minutes back.
Sam Appleton caught swim leaders Amberger and Rio Olympian Ryan Fisher on the bike, with the trio opening a handy advantage, which was engulfed by chasers Lachlan Kerin, Jack Tierney and Jake Montgomery by the time they reached T2. Appleton made his early move on the run, and was 42s ahead at the 7km mark and a minute over Fisher and Amberger at 10km. Amberger pushed into second place with 7km remaining but Appleton held off the challenge to win by 1:28, with Fisher a further 1:48 back in third.
So much to BUZZ about this week!
It was a lot like lying on a Match.com profile. When Michelle Vesterby first met her now-husband, Claus, he was the only triathlete in the pair. She would later follow him into the sport, turn pro, and earn multiple IRONMAN titles, but at the time she was training for her first marathon. Claus caught her eye, and rather than risk him losing interest, she fibbed about her triathlon experience—going so far as to buy a tri bike before their first date! Get all the details in Vesterby's blog on Triathlon World.
Canadian pro Lionel Sanders was within striking distance of the 2017 IRONMAN World Championship title—until Patrick Lange passed him in the final miles for the win. Now, Sanders is hungrier than ever. Listen in as he chats with Bob Babbitt on Babbittville Radio.
Are you one of those people that hate sharing a room during race week? Do you need your own space, and plenty of it? It may be time to think again. The men of Norway's Alpine ski team sometimes pack multiple team members into hotel rooms, and at times the men even share beds—with no complaints. Their brotherly bonds are working well; on Thursday the team took gold and silver in the Olympic Downhill. Read more about the team's unusually close camaraderie in this New York Times article.
Think your IRONMAN race Sherpa has stamina? Consider this: The parents of Swiss Olympic aerials skier Mischa Gasser traveled 17,000 miles—by bicycle, in winter—to watch their son compete. Oh, and their journey started almost a year ago, in March 2017. Read all about their adventure in the Yonhap News.
It's a fine line…between chase and race. So says IRONMAN World Champion Jan Frodeno.
IRONMAN 40th Anniversary Specialized Merchandise: Celebrate 40 Years of Dreams in style with a series of special edition 40th Anniversary IRONMAN gear coming soon and exclusively available online at Ironmanstore.com. Product will include leisure tees, tanks and hoodies as well as technical gear (cycle tops and tech tees) with 40th Anniversary Mugs and pint glasses will also be available for purchase for a limited time. In addition, select styles for the 2018 event merchandise line that can be found on site at events and will include the 40 Years of Dreams badge.


With the objective of determining what academic vocabulary students use productively, and exploring the relationship between receptive and productive academic vocabulary, this paper continues the dialog on what constitutes academic vocabulary. By adopting a set of principled criteria (ratio, dispersion, discipline specificity and range) and by approximating the procedures from a recent study of academic vocabulary, the academic vocabulary found in students' writing is identified and subsequently compared to the academic vocabulary found in published academic writing (indexical of receptive purposes). Nearly 600 words emerge as being represented significantly more frequently in students' academic writing than in their non-academic writing, demonstrating that students distinguish in their writing between academic and non-academic vocabulary. Furthermore, the investigation finds significant differences between students' productive academic vocabulary and academic vocabulary serving receptive purposes, suggesting that students' productive and receptive academic vocabulary needs are far from identical. The findings reported here are intended to serve as a tool for EAP educators working to help students develop academic vocabulary fit for purpose, as well as an incentive for EAP researchers to continue to explore the nature of academic vocabulary.


With a Canon Rebel, will this lens be ok? I'm looking to get a used manual focus lens on ebay.
I read that the Olympus Zuiko 50mm F/3.5 Macro OM Mount Manual Focus Lens would work.
Absolutely it will. I have the same lens. Do not buy anything that has fungus or other issues with it. And you need a cheap metal adapter ring, also available on ebay.
I also have the Nikon 55mm macro lens, and I think this is superior, but it is a lot more expensive. And to be honest the Olympus Zuiko is a very nice little lens.
Vivitar are also good, and if you are getting any more, e.g. a 35mm, 28mm or 24mm, their manual lenses are good products. Get adapter rings for each lens if you get several, and some rear Canon caps so yoiu do not have to take the ring on and off - they can be wear easily.
Thanks for the reply. Wasn't completely sure. I ended up picking up a Nikon Nikkor 55mm F/3.5 micro AI Manual Focus lens on Ebay. Hoping this will work!
I use the Nikkor 55mm f/3.5 micro AI manual, very happy with it. Agree with Simon, the adapter attaches to the lens, and then the whole thing goes onto the camera, so it is good to have an adapter for each lens and a Canon rear cap. I also have an Olympus OM adapter which I got because I have a few old OM lenses. So far I've only used it with a zoom, mainly for behind-the-scenes time-lapse while shoot the actual animation with a Nikon lens, but it means I can use the old OM mount 50mm and 28mm for backup if my Nikon lenses should develop a problem.
Great lens. You will not be disappointed. Reviews all class this as excellent.


Shari's wine bottles dipped in her famous dark chocolate. A layer of plastic shrink wrap is between the bottle and chocolate, a pull tab unzips breaking the chocolate away from the bottle for easy indulgence!
Dipped bottles have an eight month shelf live and make the perfect corporate gifts, wedding reception accent or hostess gift!


We are never too young to learn and implement self-care. In fact, the rapidly changing teenage brain can gain stability and become more resilient through self-care practices. The lives of teens can be drastically transformed, supported, and affirmed through self-care tools.


Cloud Theory is excited to announce a strategic partnership with Blackstone to bring FundEngine, a highly customized CRM solution built on the Salesforce platform, to the alternative asset management industry.
New York, NY, May 29, 2014. Blackstone (NYSE: BX) today announced that it has made a strategic investment in Cloud Theory, a technology consulting firm specializing in cloud-based solutions, to expand its product offering with customized Salesforce software for alternative asset managers.
"We are excited to partner with Cloud Theory to bring the Salesforce solution that works for Blackstone and make it available to the market. Managing our clients in FundEngine on the Salesforce platform allows us to continue to promote transparency with our clients across the suite of products we offer, and helps us maintain strong client relationships as we grow" said William Murphy, Chief Technology Officer of Blackstone.