YX series PMC shampoo producing machine (shampoo blending tank) is mainly suitable for preparation of liquid detergents (such as cleanser essence, shampoo and shower cream etc.). Integrating blending, dispersing, heating and cooling etc. functions, the machine is an ideal device for liquid preparation in various factories.
2.the electric rods heating way work power 47.5KW ,while the steam boiler work power only 16.5KW.a lot of energy will be consumed if choosing the former heating way.
the forth step is to storage the final products from shampoo making machine.then filling it with horizontal self suction filling machine ,about whose operation please refer to our youtube video link for furthur information https://www.youtube.com/watch?v=iOHnCVnYBw0 ,whose filling volume rangs from 60ml to 1000ml suitable for medium shampoo production .
Finaly what you need to do is to put the filled bottles on the double sides Automatic labeling machine, which can finish the labeling of any shape of bottles,either round or flat or others.


text:
10 cryptocurrencies with the ability to grow to be the subsequent crypto king in 2023
Home/Crypto/digital currency vs cryptocurrency – what's the distinction?
digital currency vs cryptocurrency – what's the distinction?
ever given that finance minister nirmala sitharaman, in the course of her 2022 budget speech, announced that the reserve bank of india (rbi) could be rolling out its digital forex, there was a lot of chatter about what exactly a digital forex is and how will it vary from cryptocurrencies inclusive of bitcoin, dogecoin and different popular tokens.
in case you've been wondering how virtual foreign money will fluctuate from cryptocurrency then this manual will help you know the entirety approximately these forms of currencies. permit's start by way of defining them first.
digital foreign money – is the digital layout of fiat foreign money which you deliver around for your pockets or withdraw from an atm. it's the equal currency that is sponsored by means of an expert, the reserve bank of india in case of indian foreign money, and can be exchanged for real currency if and whilst it's miles scheduled to be launched in 2023.
cryptocurrency – isn't sponsored by a critical parent but derives its buying strength from its network of users. technically, they are pieces of code created through 'mining' that are controlled via a digital ledger referred to as as blockchain to make sure transparency at every degree of its adventure. although coins like bitcoin and ethereum have many makes use of on the subject of nfts and the approaching metaverse, they cannot be utilised out of doors of blockchain as these are virtual belongings that may be traded however not used as a prison gentle in india.
now that we know about them, here are five most important variations between digital forex and cryptocurrency.
1 – centralisation
the largest distinction virtual foreign money and cryptocurrency is the question of who has manipulate over the monetary cost of your cash. in case of digital currency, it'd be the reserve financial institution in india or fed within the us along side the authorities, banks and other middlemen, all of whom could have to come collectively to set the price of the currency in query. that is why you'll read of the turkish lira's depreciation by over forty% in 2021 or the fall apart of monetary systems in myanmar and afghanistan as soon as the central authority is left powerless.
cryptocurrency, however, follows a obvious method right from mining to possession to transfer of crypto assets. its cost is likewise unbiased of important banking government and nearby geopolitical troubles.
2 – encryption
yet again, cryptocurrency trumps virtual forex when it comes to encryption. virtual currencies are basically e-coins that doesn't want any special indigenous strategies to encrypt them. cryptocurrencies, then again, are stored on a blockchain and the coins themselves are saved in 'wallets' that provide a far higher diploma of cyber security.
also, selecting the proper cryptocurrency change that offers the exceptional of security features and a huge variety of currencies to transact with, is the number one requirement to transact the use of cryptos. wazirx is one such crypto change that does the job reliably and one which we surprisingly propose to get started to your crypto journey. make sure to open your account here.
3 – transparency
the most important advocates for cryptocurrency will cite the transparency afforded by way of the platform. each element regarding cryptocurrency transactions is inside the public domain thanks to the presence of a decentralised ledger that statistics all the blockchain information. with virtual currency, most effective the banking authorities along with the sender and receiver are involved inside the transaction concerned. in case of warfare over any asset, cryptocurrencies are simpler to manipulate as the records are there for every body involved to peer, whereas virtual currencies should contain bureaucratic hurdles and other problems in case of any warfare. this decentralisation of records is, in fact, one of the riding forces leading to the adoption of cryptocurrencies across the world.
4 – stability
virtual foreign money is normally strong and additionally highly clean to control, thanks to having wider reputation inside the international marketplace. virtual forex, being the fiat model of authorized currency, is traded and understood by way of a tremendous majority of the population. this, in turn, makes it more solid while as compared to a brand new technology together with cryptocurrency that has commenced gaining enchantment however isn't mainstream but. delivered to that, the charge volatility of cryptocurrencies is another thing that hampers its balance whilst new tech and capabilities suggest that it's miles slowly however progressively gaining traction all round.
5– legality
most international locations, consisting of india, are now taking a look at the legality and reputation of cryptocurrencies. on the grounds that these aren't subsidized through any governing frame, most conventional frameworks don't assign any price to them. however, the speedy rise within the variety of depositors and various use instances of blockchain nowadays and the upcoming metaverse, where the best technique of payment stays cryptocurrencies, way that some sort of discussion around the legality of cryptocurrencies is bound to occur sooner than later. for now, nations around the sector are organization in backing their own fiat currencies.
now that you know which components of crypto and virtual currencies paintings for and against them, you may make an informed desire between the 2. while india's digital currency continues to be at the least a year away, through the authorities's own estimate, you may meanwhile start your crypto adventure in just a couple of minutes with wazirx, one among india's largest and most trusted cryptocurrency exchange.

redpajama_set_name: RedPajamaCommonCrawl


Believe it or not, the iPhone can fill with crash logs and make no more. We recently encountered more than one person that had a crashing app, but no new crash logs were appearing.
The crash information still appears in the device console, but no crash log is created.
Syncing the iPhone with iTunes on a desktop will remove all the old crash logs, then new crash logs can be generated.
Alternatively, you can delete the old logs with Xcode if the device is local and can be connected to USB.
This entry was posted on September 8, 2015, 7:30 pm and is filed under Regular Post. You can follow any responses to this entry through RSS 2.0. You can leave a response, or trackback from your own site.


Outside, there are three pools – a family and grown-up pool in the greenery enclosures, and a housetop lap pool, encompassed by back rub rooms, a height chamber and a contemplation room. Between the gathering rooms on the second floor, there's a completely prepared exercise center offering an every day class plan, close by a bespoke photography studio.
With regards to civilities, at that point, there's little Nasab doesn't have. However, for Zaal, the general population fill this space who will breath life into his vision. Nasab, he says, will be a spot to unite a particular kind of expert – somebody who can rouse and be enlivened, who can team up and impart, and somebody who needs to buckle down and play more enthusiastically.
These forward-looking proclamations depend on data as of now accessible to us and on the board's convictions, suppositions, evaluations, or projections and are not certifications of future occasions or results. Since such forward-looking articulations include dangers and vulnerabilities, our genuine outcomes may contrast tangibly from the forecasts in these forward-looking explanations. All forward-looking articulations are made starting today, and we accept no commitment to refresh such proclamations, regardless of whether because of new data, future occasions, or something else.


This new science series is a breath of fresh air, explaining key elements of science in a fun, straightforward way. Tom Adams's engaging, lighthearted text is perfectly complemented by the humorous, comic-book style illustrations of new talent Thomas Flintham. In Feel the Force, explore mechanics, forces, sound, light, heat and other aspects of physics, with interactive novelties and fun experiment suggestions on every spread.


This week on The #GSPodcast Stephen Knight hosts a Head-to-Head discussion on the issue of male circumcision. Defending the right of parents to circumcise their children is Sociologist and author Frank Furedi (@Furedibyte). Dr Antony Lempert (@Seculant), chair of the Secular Medical Forum will be arguing for the case against the practice.
Excellent discussion, you allowed both sides to put their point of view while avoiding one side talking over the top of the other. Both guests are to be commended as well. I personally resent the fact I was circumcised, particularly as I had no say in it and can't reverse it. I don't agree that parents should have the right to do this. We are talking about young human beings who have their own rights that should be protected, not chattels to be customised at the whim of their parents.
Love all of your podcasts. But wasting precious time on this Judeo-christian-Islamic hangup provides no universal enlightenment. I can dismiss this fetish in a few words. In their world view this almighty God created a body with parts- deal with it! As long as the fetish remains within unexciting confines of the butchers and no public laws are affected, this will die off as they also attain higher enlightnment. Amen.
The most common form of female circumcision removes the clitoral hood, a rather superfluous flap of skin. The same as male circumcision, the procedure permanently exposes the glans, causing it to become keratinized and consequently desensitized. Although they both involve the amputation of the prepuce, male circumcision removes a substantially larger portion of skin, containing a much greater number of specialized nerve receptors, and subsequently causes a much greater level of harm. The argument isn't about the level of harm that results, or the level of pain experienced, but rather the importance of a child's right to bodily autonomy. No person's freedom to practice THEIR religion overrides ANOTHER individual's right to self determination.


text:
Feature, Filmmaker Spotlight, Films
DIRECTOR SPOTLIGHT – Emrhys Cooper's on his feature THE SHUROO RETREAT "I wanted to show the dangers of following unqualified people promising quick fixes"
British director Emrhys Cooper's must see feature THE SHUROO RETREAT will be out Monday July 25th, 2022 on all streaming platforms and it is a film you don't want to miss! We have all looked for help in some form or other over the years, whether it is just a chat with a friend, seeing a therapist or looking for some kind of alternative help. THE SHUROO RETREAT questions if all Guru's are real and if we open our eyes we may find they certainly are not!
Cooper rose to fame in West End Shows like WE WILL ROCK YOU, then went on to appear in the blockbuster MAMMA MIA and then in family favourites like DESPERATE HOUSEWIVES. THE SHUROO PROCESS is his directorial debut and it certainly has left us wanting to see more of his work! We caught up with the actor, writer, dancer and director to find out more.
The film was written and produced by Cooper & Brophy, alongside executive producers Zachary Quinto and Jamie Moss for Idyllwild Pictures in association with Incline Productions. Glen Trotiner, Lynn Mancinelli and Benjamin J. Murray produced as well.
Cooper's feature directorial debut follows Parker Schafer (Fiona Dourif) a NYC journalist, frustrated with a failing publishing world and a dismal romantic life, who becomes infatuated with a charismatic guru (Brophy) and begins a journey of self-improvement. But as the old saying goes, "beware of false prophets."
What inspired you to make this film?
I grew in up in a small town in Devon that was filled with New Age teaching and wannabe guru's, unfortunately my parents fell prey to several quack doctors and guru's in some some cases to the detriment of their health. I wanted to show the dangers of following unqualified people promising quick fixes.
For people who haven't seen the film, can you describe it?
Well, it's about a NYC journalist's who's life crashes and burns, she then becomes infatuated with a celebrity guru, taking her on a wild journey of love and grand larceny. The Shuroo Retreat explores the dangers of the cultish self-help industry and what it is like to fall prey to its promises of transformation.
The Shuroo Retreat explores the dangers of the cultish self-help industry and what it is like to fall prey to its promises of transformation.
You have a fantastic cast, what was it like working with such a great cast and what is your most memorable moment?
I feel extremely fortunate to have gotten such an accomplished group of actors in my directorial debut. The choreographed elements of the masked dance stick out in my mind the most.
The film features Fiona Dourif, Donal Brophy, Tommy Dorfman, Emrhys Cooper, Rainey Qualley, Olivia Sui, Hakeem Kae-Kazim, Jeff Hephner, Cornelia Guest, and more.
What was it like to both direct and star in the film?
Very difficult to be honest. Not sure I need to do that agin but ultimately rewarding when I see the finished product. It'd quite confusing to be behind the camera and have to jump in front.
What would you like people to take from the film.
It's important to take a step towards healing, no matter where it leads you have invested in yourself.
We have a great podcast in works exploring LGBTQ historical figures and in the process of developing my award winning short TROPHY BOY into a TV series… As well and many other exciting projects all seen in detail on the website for Idyllwild Pictures.
Editor July 22, 2022 July 22, 2022 Cornelia Guest, Donal Brophy, Emrhys Cooper, Film and Television Business, Film and TV Business, Film Business, Fiona Dourif, Hakeem Kae-Kazim, Idyllwild Pictures, Jeff Hephner, Olivia Sui, Rainey Qualley, THE SHUROO RETREAT, Tommy Dorfman, Zachary Quinto
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text:
(-) Conflict & Conflict Resolution--Governance (123)
(-) Energy--Energy security (52)
(-) Economics & Global Affairs--Emerging Markets Development (12)
Belfer Center Spring 2019 Newsletter
Read more about Belfer Center Spring 2019 Newsletter
The Spring 2019 issue of the Belfer Center newsletter features two major reports: A Vision for Nuclear Security, from the Project on Managing the Atom, and NATO in Crisis, a 70th anniversary report from former NATO Ambassadors Nicholas Burns and Douglas Lute. The newsletter also highlights Center Korea scholars' reactions to the shortened Trump-Kim Summit in Hanoi, and some takeaways from nuclear experts who recently examined samples of Iranian nuclear-related documents spirited out of Iran by a clandestine Israeli intelligence operation.
And there's much more.
cdc.gov/phil
Analysis & Opinions - Belfer Center for Science and International Affairs, Harvard Kennedy School
How to Deal with Increasingly Complex Safety-Critical Technologies
Najmedin Meshkati
Sébastien Philippe
Read more about How to Deal with Increasingly Complex Safety-Critical Technologies
The authors analyze the 1979 Three Mile Island nuclear accident and the recent back-to-back crashes of two Boeing 737 Max jets and make policy recommendations for the regulation of increasingly complex technologies.
WGBH
Analysis & Opinions - WGBH
Former Ambassador Nicholas Burns Discusses Trump's Foreign Policy
Read more about Former Ambassador Nicholas Burns Discusses Trump's Foreign Policy
It's been six months since President Donald Trump and North Korean leader Kim Jong Un said they came to an agreement on denuclearization, but new satellite images published this week by an independent Washington think tank showed at least 13 previously undeclared missile operating bases in North Korea.
Analysis & Opinions - MSNBC
How Will Trump's Iran Deal Decision Impact Foreign Policy?
Jake Sullivan
Read more about How Will Trump's Iran Deal Decision Impact Foreign Policy?
Before President Trump announces his decision on the Iran Deal, Former US Ambassador to NATO Nick Burns and Former Senior Policy Advisor for Hillary Clinton's Campaign Jake Sullivan join Andrea Mitchell to discuss what this decision could mean for foreign policy.
Fox Business Network
Analysis & Opinions - Fox News
Looking at a White House in disarray
Read more about Looking at a White House in disarray
Nicholas Burns, former State Department undersecretary, on the tensions between President Trump and Attorney General Jeff Sessions and Trump's handling of U.S. foreign policy.
Former Deputy Secretary of Energy Elizabeth Sherwood-Randall Named Senior Fellow With Harvard's Belfer Center
Elizabeth D. Sherwood-Randall
Read more about Former Deputy Secretary of Energy Elizabeth Sherwood-Randall Named Senior Fellow With Harvard's Belfer Center
Former Deputy Secretary of Energy Elizabeth Sherwood-Randall is joining Harvard Kennedy School's Belfer Center for Science and International Affairs as a Senior Fellow, the Center announced today. Sherwood-Randall, who has served in the White House and Departments of Energy and Defense, is returning to the Center where she worked in the 1990s to help establish two pioneering projects – the Strengthening Democratic Institutions Project with Graham Allison, who this month stepped down as the Center's director, and the Preventive Defense Project with Ash Carter, the former Secretary of Defense who is the new Belfer Center director.
News - Belfer Center for Science and International Affairs, Harvard Kennedy School
Q&A with Elizabeth Sherwood-Randall
Read more about Q&A with Elizabeth Sherwood-Randall
Elizabeth Sherwood-Randall, former Deputy Secretary of Energy who has served in high-level positions at the White House and Pentagon, joined Harvard Kennedy School's Belfer Center as a non-resident Senior Fellow in July. Sherwood-Randall is returning to the Kennedy School where she previously collaborated with Ash Carter, the Belfer Center's newly appointed director, and Graham Allison, who stepped down as Center director this month. We asked Sherwood-Randall to give us some background on her Harvard connections, why she returned, and what she hopes to accomplish as a Senior Fellow.


🌷 Bye Bye Winter And Hello Spring!!!!!!
🌷 The Vernal (Spring) Equinox falls on 3/20/19, at 5:58 P.M.
🗣 Legand has it that you can stand an egg 🥚 on its end ONLY during the Vernal Equinox.
➡ Try this yourself and show 🎥 us know what happens.


text:
Megadeth declare they are officially "back" following Dave Mustaine's cancer battle
Jon Hadusek
Consequence of Sound January 8, 2020
The post Megadeth declare they are officially "back" following Dave Mustaine's cancer battle appeared first on Consequence of Sound.
It's official: Megadeth have returned following frontman Dave Mustaine's battle with cancer. The thrash metal legends posted on Twitter that they're "back" and ready to play shows after postponing all 2019 tour dates when Mustaine was diagnosed with throat cancer last June.
"Megadeth is back!" the band exclaimed. "We can't wait to see and play for you all on the Killing Road in 2020! What songs do you want to hear?"
Perhaps a couple of "crushing" new songs will make it into the setlists for Megadeth's upcoming European shows with Five Finger Death Punch, kicking off later this month. Mustaine previously said that he hopes to release new material in time for the winter tour.
Meanwhile, bassist David Ellefson reported in October that Mustaine had completed his cancer treatments, and that the band would return to work on their new album after the frontman fully recovered.
"Once he's through that process, we're gonna just let that take as much time as it needs," Ellfeson said, "and then we'll resume with the album. I'd like to hope maybe 2020 we'll be able to get a new album out."
If today's tweet is any indication, Mustaine appears to be healthy enough to tour and record. See the full post below.
Megadeth is back! We can't wait to see and play for you all on the Killing Road in 2020! What songs do you want to hear? pic.twitter.com/RZOcoaHwfG
— Megadeth (@Megadeth) January 7, 2020
Rage Against the Machine to headline Boston Calling 2020: Sources
Jason Segel and Paul Rudd pay tribute to Rush drummer Neil Peart
Subscribe to Consequence of Sound's email digest and get the latest breaking news in music, film, and television, tour updates, access to exclusive giveaways, and more straight to your inbox.


text:
\section{Introduction} The development of lasers has revitalized
atomic, molecular, chemical, and optical physics.  The interaction of
intense laser pulses with matter gives rise to a wealth of phenomena that are nonlinear in both the laser intensity and the number of photons involved, examples being multiphoton ionization (MPI), above-threshold
ionization (ATI), or tunneling ionization (see, e.g.,
\cite{Milosevic2006} for a review). While for weak laser fields MPI
could still be tackled in a perturbative fashion where each
additionally absorbed photon requires the next-order, conventional
perturbation theory becomes inadequate for stronger fields due to the
lack of a small parameter and very pronounced AC-Stark
effects \cite{delone2000multiphoton}. Instead, the so-called strong-field approximation (SFA) (see, e.g.,
\cite{Milosevic2006,Popruzhenko2014a} for a recent review) became the work horse of
choice and particularly insightful when interpreted in terms of
quantum orbits \cite{Milosevic2006,Popruzhenko2014a}. For instance, ATI peaks
separated in energy by $\hbar\omega$ can be understood as the
interference of quantum orbits of electrons emitted in subsequent
laser cycles (inter-cycle interference) while interfereing quantum
orbits originating from the same laser cycle (intra-cycle
interference) lead to other features in photoelectron spectra (PES) \cite{Arbo10},
such as holographic side lobes \cite{Huismans2011,huismansprl2012}.

Patterns in the photoelectron spectra clearly depend on the laser
pulse and the target. The dependency on the particulars of the laser
field allow for the control of the ionization dynamics or the precise
experimental characterization of the laser pulse \cite{chini2014}. The dependency on
the target opens up the possibility to image the system employing its
own electrons \cite{Blaga2012}.

In this work, we do not consider the PES themselves but the {\em
change} of the momentum-resolved yield as function of a the relative phase $\varphi$ between the
$\omega$ and the $2\omega$ component of a colinearly polarized
two-color pulse with vector potential (in dipole approximation)
\begin{equation}\label{vp} \textbf{A}(t) = A_0(t)\Big[\sin \omega t +
\xi \sin(2 \omega t + \varphi) \Big]{\bf e}_{z},
\end{equation} where $\xi$ is a relative field amplitude, and $A_0(t)$
is the envelope of the laser pulse. Note that if the ratio of $2\omega$ to $\omega$ component of the vector potential is $\xi$, the ratio of the corresponding electric field components is $2\xi$ because $\vekt{E}=-\partial_t\vekt{A}$. The ratio in intensities then is $(2\xi)^2$. Below we will consider $\xi=0.05$, i.e., the $2\omega$ component of the electric field is 10\% of the fundamental, and the intensity ratio is 1\%.

A plethora of two-color studies have been performed recently, with different combinations of laser frequencies and polarizations
\cite{Gong2017,EickeLein2017,Busulad2017,Vvedenski2017,Zhang2017,Hamilton2017,Song2017,Natan:16,Li:16,Yu2016,mancuso2016,richter2016,Das2016,petersson2016,Zheng2015,Skrusz2015,ArboKitzler2014}.
Important foreseeable applications of two-color fields are the efficient generation of THz radiation from plasmas \cite{Zhang2017} or the control of strong-field phenomena by steering the electron emission \cite{ZhoOE11}, for instance. Atoms and molecules in two-color fields are also interesting in themselves as they allow a deeper understanding of the ionization dynamics due to the high sensitivity of strong-field observables to the detailed shape of the electric field, which is modified by the relative phase $\varphi$  on a sub-cycle time scale. Relative-phase dependent measurements are thus  a more challenging, stringent test for theory and, perhaps most
importantly, offer the possibility to distinguish coherent and incoherent
contributions to PES or other observables. Here, ``coherent'' and ``incoherent'' mean that
the ionization dynamics that lead to photoelectrons with a certain
final momentum in PES do depend or do not depend on the precise
shape of the electric field of the laser, and thus on the relative
phase $\varphi$. The subcycle ionization dynamics in few-active
electron systems such as atoms or small molecules are expected to be
coherent in this sense while thermal enmission from larger systems is
expected to be incoherent. Before we aim at complex targets though, we
need to understand the canonical, ``textbook'' phase-of-the-phase (PP) spectra originating
from coherent electron emission. In Ref.~\cite{Skrusz2015}, phase-of-phase spectra
were found to show a typical structure of two overlapping clubs due to
rescattering in strong laser fields. In this work we investigate phase-of-phase spectra at lower laser
intensities, i.e., in the multiphoton ionization (MPI) regime.

The paper is organized as follows:  The fundamental idea behind phase-of-the-phase spectroscopy is introduced and a generic experimental result for Xe is presented in Sec.~\ref{sec:experiment}. Simulation results and the derivation of the ionization rate for a two-color pulse, both based on the SFA, are presented in Sec.~\ref{theory}, followed by a discussion in Sec.~\ref{disc}. We briefly summarize and give an outlook in Sec.~\ref{concl}.

Atomic units are used unless
indicated otherwise. The dipole approximation is valid for the laser
parameters under study and applied throughout.

\section{Experimental result and phase-of-the-phase analysis} \label{sec:experiment}
Details of the experimental setup to measure phase-sensitive signals
from two-color laser pulse excitations of atoms and molecules has been
described previously \cite{Skrusz2015}. Briefly, a Ti:sapphire laser
system produces near-infrared pulses of energy $E_\mathrm{L} =2.5$\,mJ and
$\lambda=794$\,nm with a pulse duration of 180\,fs at a repetition
rate of 1\,kHz. To sculpture the pulses on the time scale of the
electric field oscillation the fundamental is superimposed by a weak
second harmonic field with an intensity ratio $I_{2\omega}/I_\omega=0.01$. The temporal
overlap between fundamental and second harmonic is controlled by birefringent
calcite crystals and two glass wedges. Additional wave plates are used
to align the polarization axes parallel to each other.  The wedges
are mounted on piezo-driven motors to achieve sub-cycle control over
the relative phase $\varphi$ between $\omega$ and $2\omega$ component. A
concave silver-mirror with a focal length of 250\,mm focuses the
pulses into the interaction region of a homebuilt velocity map imaging (VMI)
electron spectrometer~\cite{SkrRSI14}, giving pulse intensities of
$I_\omega \simeq 5\times 10^{13}$\,W\,cm$^{-2}$. Rare gases enter as an
effusive beam from a nearby capillary.

Figure~\ref{fig:VMIsnapshot} shows a typical snapshot of the VMI
screen for such a two-color experiment on xenon atoms.
ATI rings and the previously studied ``carpet'' structure
\cite{Korneev2012} are clearly visible. However, because the $2\omega$
component is just a weak perturbation, no big changes are seen on the
VMI screen with the naked eye when the relative phase $\varphi$ is
changed.
\begin{figure}
    \includegraphics[width=0.75\columnwidth]{snapshotcut.png}
    \caption{Screenshot of the VMI detector during a colinearly
polarized two-color experiment with Xe.  Laser
polarization in horizontal direction. Laser parameters are given in the text. ATI rings separated by
$\hbar\omega$ in energy and the ``carpet'' structure \cite{Korneev2012} are clearly visible.  }
    \label{fig:VMIsnapshot}
\end{figure}
 The idea behind phase-of-the-phase spectroscopy is to study systematically the {\em
change} in the photoelectron yield as a function of the relative phase
$\varphi$ (or any other periodic parameter, e.g., the carrier-envelope
phase \cite{Zhereb2012}).  Assuming that the momentum-resolved yield
$Y(\vekt{p},\varphi)$ behaves predominantly as
\begin{equation} Y(\vekt{p},\varphi) \simeq Y_0(\vekt{p}) + \Delta
Y_1(\vekt{p}) \cos[\varphi+\Phi_{1}(\vekt{p})] \label{yield}
\end{equation} for most final photoelectron momenta $\vekt{p}$, the change in the
yield can be characterized by just two functions of $\vekt{p}$: the relative phase
contrast (RPC) $\Delta Y_1(\vekt{p})\geq 0$ and the phase of the phase (PP) $\Phi_1(\vekt{p}) \in [-\pi,\pi)$ that
tells us whether the yield changes, e.g., $\pm\cos$-like with
$\varphi$ or $\pm\sin$-like. Technically, phase of phase and relative phase contrast can be quickly
determined by fast-Fourier-transforming $Y(\vekt{p},\varphi)$ with
respect to $\varphi$ for each $\vekt{p}$. The yield may
actually change with twice the relative phase for certain final
momenta $\vekt{p}$, i.e., $\sim\Delta Y_2(\vekt{p}) \cos[2\varphi+\Phi_2(\vekt{p})]$. In fact, this is
the case in leading order $O(\xi^2)$ for electron emission
perpendicular to the polarization direction because $\Delta
Y_1=0$ there.  However, in this work we limit our discussions to
the fundamental PP $\Phi_1$, i.e., to order $O(\xi)$, as will be shown in
Section~\ref{theory} below.

Figure~\ref{fig:exp:RPCandPP} shows the experimental RPC and PP
spectra for xenon, determined from a series of snapshots for varied relative phase $\varphi$ like the one
in Fig.~\ref{fig:VMIsnapshot}. For a fixed relative phase the average of $10000$ PES is taken. The relative phase is sampled in steps of   $\simeq 2\pi/70$.  A checkerboard pattern in the PP along the ATI rings is clearly visible.
The color coding can be cyclically shifted because only the change in
the relative phase is controlled in the experiment, not its absolute
value. We chose the color-coding such that the checkerboard pattern is
red and blue, representing $\pm\sin$-like changes in the yield
$Y(\vekt{p},\varphi)$ according to the pulse form \eqref{yield} assumed in
the theoretical analysis.

\begin{figure}
    \includegraphics[width=0.8\columnwidth]{RPCandPOPexp.png}
    \caption{Experimental RPC $\Delta Y_1(\vekt{p})$ (a) and PP
$\Phi_{1}(\vekt{p})$ (b) spectra for Xe. Parameters as for
Fig.~\ref{fig:VMIsnapshot}, given in the text. A checkerboard pattern oriented along the ATI rings is visible in the PP spectrum (b).}
    \label{fig:exp:RPCandPP}
\end{figure}

\section{Theory} \label{theory} We apply the SFA for the so-called direct
electrons, i.e., those that do not rescatter at the parent ion.
In length gauge, the SFA matrix element reads \cite{Milosevic2006,Popruzhenko2014a} \begin
{equation}\label{direct} M^{(\text{SFA})}_{\textbf{p}} = -\mathrm{i}
\int^{\infty}_{-\infty}\langle
\Psi^{\text{GV}}_{\textbf{p}}(t)|\textbf{r}\cdot
\textbf{E}(t)|\Psi_{0}(t)\rangle \, \mathrm{d} t
\end {equation} where
\begin {equation}\label{volkovstate}
|\Psi^{\text{GV}}_{\textbf{p}}(t)\rangle=
\mathrm{e}^{-\mathrm{i}S_{\textbf{p}}(t)}|\textbf{p}+
\textbf{A}(t)\rangle
\end {equation} is a Gordon-Volkov (GV) state, i.e., a solution to the
time-dependent Schr\"odinger equation
$\mathrm{i}|\dot{\Psi}^{\text{GV}}_{\textbf{p}}(t)\rangle =
[\vekt{p}^2/2 +
\vekt{r}\cdot\vekt{E}(t)]|\Psi^{\text{GV}}_{\textbf{p}}(t)\rangle$ without
binding potential but laser only, $|\Psi_{0}(t)\rangle =
\exp(\mathrm{i}I_{\mathrm{p}} t) |\Psi_{0}(0)\rangle$ is the initial bound state,
and
\begin{equation} S_{\textbf{p}}(t)=\frac{1}{2} \int^{t}[\textbf{p}+
\textbf{A}(t')]^{2} \, \mathrm{d} t'
\end{equation} is the Coulomb-free, classical action. In dipole approximation, the PES $|
M^{(\text{SFA})}_{\textbf{p}}|^2$ is azimuthally symmetric about the
laser polarization axis in $\vekt{e}_z$ direction. For illustration, PES
calculated with the SFA for laser intensity $I = 5 \times
10^{13}\,$W/cm$^2$, $\lambda=800$\,nm ($\omega=0.057$), $20$-cycle $\sin^2$
pulse, $\xi=0.05$, relative phases $\varphi=0,\pi/2,3\pi/2$, and
$I_{\mathrm{p}}=0.445$ (Xe) are shown in Fig.~\ref{fig:sfa:matrixelem}. The
initial state $|\Psi_{0}(0)\rangle$ affects the result only as a
preexponential form factor $\langle \vekt{p} + \vekt{A} | \vekt{r}
|\Psi_{0}(0)\rangle \cdot \vekt{E}(t)$ \cite{Milosevic2006,Popruzhenko2014a}. For simplicity, we chose a hydrogen-like 1s state for
$|\Psi_{0}(0)\rangle$ with $I_{\mathrm{p}}$ adjusted to Xe.
  For all $\varphi$ ATI rings are clearly visible. For $\varphi=0$
(or $\pi$), the SFA-PES is left-right symmetric (i.e., invariant under
the transformation $p_z \to -p_z$). Instead, for $\varphi=\pi/2$ and
$3\pi/2$ the weak $2\omega$ component of the laser field introduces a
visible left-right asymmetry: the ATI peaks appear to be more pronounced and shifted along
the ATI rings. These shifts could be reproduced extending the quantum orbit approach and the calculation of the curves of destructive interference as outlined in \cite{Korneev2012} to two-color fields. However, we aim at a closed analytic expression for the ionization probability as a function of the relative phase in this work and thus follow a different route.

\begin{figure}
    \includegraphics[width=0.8\columnwidth]{sfaforthreedifferentphi.png}
    \caption{ Logarithmically color-coded SFA-PES for $I_{\mathrm{p}}=0.445$ (Xe), vector potential amplitude
$A_0=2/3$, $\omega=0.057$, $20$-cycle $\sin^2$ pulse, $\xi=0.05$,
and $\varphi=0$, $\pi/2$, $3\pi/2$, calculated from
\eqref{direct}.} \label{fig:sfa:matrixelem}
 \end{figure}

Figure~\ref{fig:sfa:matrixelemRPCandPP} shows the RPC $\Delta Y_1(\vekt{p})$  and the PP $\Phi_1(\vekt{p})$
 for the parameters of
Fig.~\ref{fig:sfa:matrixelem}. A checkerboard pattern similar to the one in the experimental PP spectrum in   Fig.~\ref{fig:exp:RPCandPP}b is observed, at least for sufficiently big lateral momenta $|p_x|$. The PP signature for small momenta is different because of the neglect of Coulomb effects on the emitted electrons in the SFA \cite{Bauer2006a,Popruzhenko2014a}. The fact that there is a checkerboard pattern in PP spectra at all is simple to understand: if an ATI
peak moves along its ATI ring, the yield increases in regions where
previously was less probability and decreases at the initial location. As a consequence, only two discrete PPs show up. Why the yield within an SFA
treatment behaves $\pm\sin\varphi$-like and not with some other pair
of PPs is less obvious but will be derived analytically in the following.

\begin{figure}
    \includegraphics[width=0.8\columnwidth]{sfamatrixelemRPCandPP.png}
    \caption{RPC (a) and PP (b) calculated from PES for 20 values of  $\varphi\in
[0,2\pi)$ and the parameters of
Fig.~\ref{fig:sfa:matrixelem}. } \label{fig:sfa:matrixelemRPCandPP}
 \end{figure}

In order to obtain an analytical result we work in velocity gauge and
consider long flat-top pulses of vector potential amplitude $A_0$ that are switched on and off
at $\mp\infty$.  It is known that the SFA is plagued by gauge
non-invariance, leading, in general, to different PES for velocity
gauge (with $\vekt{p}\cdot\vekt{A}(t)$ as the interaction term) and length
gauge (with $\vekt{r}\cdot\vekt{E}(t)$, with the electric field
$\vekt{E}=-\partial_t\vekt{A}$) \cite{Bauer2005}. However, in this work we use an
$1$s-state as the inital state for the SFA and tune the
ionization potential $I_{\mathrm{p}}$ to the experimental value. In that case
there is no visible difference between length and velocity gauge PES obtained numerically from the SFA.
The SFA matrix element relevant for the ionization rate
$\Gamma_\vekt{p}$ can then be written in the form \cite{Reiss1980}
\begin{equation}\label{mvelocity} {M'}^{(\text{SFA})}_{\textbf{p}} =
\mathrm{i}\Psi_{0}(\textbf{p})\left( \frac{p^{2}}{2} + I_{\mathrm{p}}\right)
\int^{\infty}_{- \infty} \mathrm{d}
t~\mathrm{e}^{\mathrm{i}S_{\textbf{p},I_{\mathrm{p}}}(t)},
\end{equation} with $\Psi_{0}(\textbf{p}) = \langle
\textbf{p}|\Psi_{0}\rangle$ and
\begin{equation}\label{s} S_{\textbf{p},I_{\mathrm{p}}}(t)=
\int_{-\infty}^{t}\left\{\frac{1}{2}[\textbf{p}+ \textbf{A}(t')]^{2} +
I_{\mathrm{p}} \right\}\, \mathrm{d} t'.
\end{equation} Inserting \eqref{vp} with $A_0(t)=A_0$ into \eqref{s},
\begin{align}\label{ss} S_{\textbf{p},I_{\mathrm{p}}}(t) = &
\left(\frac{p^{2}}{2} + I_{\mathrm{p}} + U_{\mathrm{p}}\right)t\\ & - \frac{A_0
p_z}{\omega}\sin\left(\omega t+{\pi}/{2}\right) + \frac{A_0^2}{8
\omega} \sin\big[2(\omega t +\pi/2)\big] \nonumber \\ &
-\frac{A_0\xi}{\omega}\bigg[\frac{p_z}{2} \cos(2\omega t + \varphi) +
\frac{A_0}{6} \sin(3\omega t + \varphi) \nonumber \\ & \qquad\qquad -
\frac{A_0}{2} \sin(\omega t + \varphi)\bigg] + {\cal{O}}(\xi^2)
\nonumber
\end{align} is obtained. Here, $U_{\mathrm{p}}=A_0^2/4$ is the ponderomotive energy.  With the help of the generalized Bessel functions
$J_{n}(u, v)$,
\begin {align} \mathrm{e}^{\mathrm{i} [ u\sin \phi + v \sin(2\phi)]} =
& \sum^{\infty}_{n=-\infty} \mathrm{e}^{\mathrm{i}n\phi}J_{n}(u, v),
\\ J_n(u,-v) = & (-1)^n J_{-n}(u,v),
\end{align} we can evaluate the matrix element \eqref{mvelocity},
neglecting terms of order ${\cal{O}}(\xi^2)$, as
\begin{align}\label{matrix} {M'}^{(\text{SFA})}_{\textbf{p}} = & 2\pi
\mathrm{i} \Psi_{0}(\textbf{p})\bigg(\frac{p^2}{2} + I_p\bigg) \\ &
\times \sum^{\infty}_{n=-\infty}\mathrm{i}^{n}
\delta\Big(\frac{p^2}{2} + I_{\mathrm{p}} + U_{\mathrm{p}} - n\omega \Big) \Bigg\{ J_{n}
\nonumber \\ & + \frac{\mathrm{i}A_0 \xi}{4\omega}\bigg[\Big(A_0
J_{n+1}+ p_zJ_{n+2} + \frac{A_0}{3} J_{n+3}\Big)
\mathrm{e}^{\mathrm{i}\varphi} \nonumber \\ & + \Big( A_0J_{n-1} +
p_zJ_{n-2} +\frac{A_0}{3} J_{n-3}\Big) \mathrm{e}^{-
\mathrm{i}\varphi} \bigg] \Bigg\} . \nonumber
\end{align} Here we suppressed for brevity the arguments of all the generalized
Bessel functions, i.e., \begin{equation} J_n=J_n(u,v), \quad u=-\frac{p_zA_0}{\omega}, \quad v= -\frac{U_{\mathrm{p}}}{2\omega}. \end{equation}
For the rate follows, analogously to the one-color calculation in, e.g., Refs.~\cite{Reiss1980,Mulser2010},
\begin{align}\label{bessel} \Gamma_\vekt{p} = &
2\pi|\psi_{0}(\textbf{p})|^{2}\left(\frac{p^2}{2}+ I_{\mathrm{p}}\right)^{2} \\ &
\times \sum^{\infty}_{n=-\infty} \delta \Big(\frac{p^2}{2} + I_{\mathrm{p}} + U_{\mathrm{p}}
- n \omega \Big) \Bigg\{ J_{n}^{2} - J_{n}\xi \sin \varphi \nonumber
\\ & \times \Bigg[4 v( J_{n-1} - J_{n+1}) + \frac{u}{2} (J_{n-2} -
J_{n+2} ) \nonumber \\ & + \frac{4v}{3}(J_{n-3} - J_{n+3} ) \Bigg]
\Bigg\}.
\end{align} We can eliminate the terms $\sim J_{n\pm 3}$ using the property of the generalized Bessel functions $2nJ_n
= u(J_{n-1}+J_{n+1}) + 2v (J_{n-2} - J_{n+2})$, which yields
\begin{align}\label{bessel2} \Gamma_\vekt{p} = &
2\pi|\psi_{0}(\textbf{p})|^{2}\left(\frac{p^2}{2}+ I_{\mathrm{p}}\right)^{2}
\sum^{\infty}_{n=-\infty} \delta \Big(\frac{p^2}{2} + I_{\mathrm{p}} \\ & + U_{\mathrm{p}} -
n \omega \Big) \Bigg[ J_{n}^{2} + \Xi_n(u,v) \sin \varphi
\Bigg]\nonumber
\end{align} where
\begin{align}\label{K} \Xi_n(u,v) = & - \frac{4 \xi J_{n}}{3} \Bigg[(4
v + n) ( J_{n-1} - J_{n+1}) \\ & - (J_{n-1} + J_{n+1} ) -
\frac{u}{8}(J_{n-2} - J_{n+2} ) \Bigg] . \nonumber
\end{align} For $\xi=0$, the known result \cite{Reiss1980} for the PES without the
$2\omega$ component is obtained. The rate \eqref{bessel2} has indeed
the same structure as the assumed yield in \eqref{yield}, that is
\begin{equation} \Gamma_\vekt{p} = \Gamma_{0\vekt{p}} + | \Delta
\Gamma_\vekt{p} | \cos[\varphi+\Phi_1(\vekt{p})],
\end{equation} with the RPC $| \Delta \Gamma_\vekt{p} |$ where
\begin{align}\label{rpcrate} \Delta \Gamma_\vekt{p} = &
2\pi|\psi_{0}(\textbf{p})|^{2}\left(\frac{p^2}{2}+ I_{\mathrm{p}}\right)^{2} \\ &
\times \sum^{\infty}_{n=-\infty} \delta \Big(\frac{p^2}{2} + I_{\mathrm{p}} + U_{\mathrm{p}}
- n \omega \Big) \Xi_n(u,v), \nonumber
\end{align} and the PP $\Phi_1(\vekt{p})=\pm \pi/2$, depending on the
sign of $\Delta \Gamma_\vekt{p}$.  Evaluating the rate \eqref{bessel2}
 gives very similar results for PP and RPC as in
Fig.~\ref{fig:sfa:matrixelemRPCandPP}, as shown in
Fig.~\ref{fig:sfa:besselian}. The checkerboard structure is more pronounced in the analytical result  because of the flat-top, infinite-pulse assumption on which \eqref{bessel2} is based. For the numerical evaluation, the $\delta$ distribution in  \eqref{bessel2}  was replaced by a Gaussian $\exp[-(p^2/2+I_{\mathrm{p}}+U_{\mathrm{p}}-n\omega)^2/a^2]/a\sqrt{\pi}$ with $a=1/20$, and the sum over $n$ was restricted to $\sum_{n=-30}^{30}$.
\begin{figure}
    \includegraphics[width=0.8\columnwidth]{RPCandPOPsfaanalytical.png}
    \caption{RPC (a) and PP (b) spectra calculated using the flat-top,
infinite pulse SFA result for the rate Eq.~\eqref{bessel2}.}
    \label{fig:sfa:besselian}
\end{figure}

\section{Discussion} \label{disc}
The characteristic
checkerboard pattern in the momentum-resolved phase-of-the-phase spectra is
found in both theoretical and experimental results for xenon.
As mentioned above, this
pattern is related to above-threshold ionization peaks that are
shifted with varying relative phase. While the analytical calculation
based on the strong-field approximation predicts only
$\pm\sin\varphi$-like behavior of the yield for a $\sin\omega t +
\xi\sin(2\omega t + \varphi)$-like vector potential \eqref{vp}, the experiment
shows a more complex PP signature. Also, the experimental relative phase contrast is more oriented along the polarization axis than in the SFA. This clearly points towards the importance of Coulomb effects, which are expected to be the more pronounced the lower the photoelectron energy \cite{Bauer2006a,Popruzhenko2008}.
Other
sources of discrepancy between SFA and experiment are due to focal
averaging, the projection onto the VMI detector plane in the measured PES \cite{vrakk2001}, possible resonance-enhanced multiphoton ionization (REMPI) \cite{Gong2017} and Freeman resonances \cite{Freeman91,Schyja98}. Comparison with PES from the numerical solution of the
time-dependent Schr\"odinger equation will be the subject of future
work. Preliminary TDSE results show that the PES also display
checkerboard patterns but also PP other than $\pm \sin$-like, as in the
experiment. However, achieving agreement in all details between TDSE and
experiment is challenging, even in the case of atomic hydrogen \cite{Kielp2014}.

\section{Summary and outlook} \label{concl}
An analytical expression for the ionization rate
in a two-color ($\omega$-$2\omega$), colinearly polarized laser field
was derived using the strong-field approximation. The change in the
yield as a function of the relative phase $\varphi$ between the two
color components was analyzed in the multiphoton regime using the
recently introduced phase-of-the-phase spectroscopy. A characteristic
checkerboard pattern in the momentum-resolved phase of the phase was
found in both theoretical and experimental results for xenon.

The visibility of the checkerboard pattern in the phase-of-the-phase spectra is
clearly related to the presence of above-threshold ionization peaks. Now, imagine an
experiment where photoelectron spectra from many-electron systems such as larger
molecules, clusters, fullerenes, droplets, nanospheres, or solids are
measured. Because of the various relaxation channels, above-threshold ionization peaks or
other patterns in photoelectron spectra based on the interference of different electron
pathways may be masked by delayed or even thermal electron emission,
leading to insipidly Maxwellian-like spectra. Phase-of-the-phase
spectroscopy effectively removes these incoherently emitted electrons
from the spectrum because incoherent emission is independent of the
relative phase. This idea was applied to the electron emission from
SiO$_2$ nanospheres due to the interaction with strong, few-cycle
laser fields \cite{Zhereb2012} where the phase-of-phase analysis was performed with respect to
the carrier-envelope frequency instead of the relative phase between
the two colors in a two-color laser field. Clearly, phase-of-the-phase spectroscopy
can be applied with respect to any periodic ``knob'' that can be controlled in an
experiment.

\section*{Acknowledgment} This work was supported by the SFB 652 and
projects BA 2190/8 and TI 210/7 of the German Science Foundation (DFG).

redpajama_set_name: RedPajamaArXiv


YouTube is now integrated with Google+ and if you want to setup a channel or do anything on YouTube, you will need to have a Google+ account. One of the most powerful benefits of this integration for you as a business owner is that whenever someone comments on a video, that video could potentially show up on their news feed. They would need to have chosen the option for the video to actually show up.
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text:
IBM Bluemix Mobile Services - Client SDK Swift Push
===================================================

[![Build Status](https://travis-ci.org/ibm-bluemix-mobile-services/bms-clientsdk-swift-push.svg?branch=master)](https://travis-ci.org/ibm-bluemix-mobile-services/bms-clientsdk-swift-push)
[![Codacy Badge](https://api.codacy.com/project/badge/Grade/08bd0c46c0ae4485a3abc0fd8dffa4cf)](https://www.codacy.com/app/ibm-bluemix-mobile-services/bms-clientsdk-swift-push?utm_source=github.com&utm_medium=referral&utm_content=ibm-bluemix-mobile-services/bms-clientsdk-swift-push&utm_campaign=Badge_Grade)
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[![CocoaPods Compatible](https://img.shields.io/cocoapods/v/BMSPush.svg)](https://github.com/ibm-bluemix-mobile-services/bms-clientsdk-swift-push.git)
[![](https://img.shields.io/badge/bluemix-powered-blue.svg)](https://bluemix.net)
[![CocoaPods](https://img.shields.io/cocoapods/dt/BMSPush.svg)](https://cocoapods.org/pods/BMSPush)

This is the Push component of the Swift SDK for [IBM Bluemix Mobile Services](https://console.ng.bluemix.net/docs/mobile/index.html).

## Contents

This package contains the Push components of the Swift SDK.
* Push Registration and Unregister
* Subscribing and Unsubscribing for Tags

## Requirements

* iOS 8.0+
* Xcode 7.3, 8.0
* Swift 2.3 - 3.0
* Cocoapods or Carthage

## Installation

The Bluemix Mobile Services Swift SDKs are available via [Cocoapods](http://cocoapods.org/) and [Carthage](https://github.com/Carthage/Carthage).

### Cocoapods
To install BMSPush using Cocoapods, add it to your Podfile:

```ruby
use_frameworks!

target 'MyApp' do
    platform :ios, '8.0'
    pod 'BMSCore', '~> 2.0'
    pod 'BMSPush', '~> 3.0'
end
```
From the Terminal, go to your project folder and install the dependencies with the following command:

```
pod install
```

#### Swift 2.3

Before running the `pod install` command, make sure to use Cocoapods version [1.1.0.beta.1](https://github.com/CocoaPods/CocoaPods/releases/tag/1.1.0.beta.1).

#### Swift 3.0

Before running the `pod install` command, make sure to use Cocoapods version [1.1.0.beta.1](https://github.com/CocoaPods/CocoaPods/releases/tag/1.1.0.beta.1).

For apps built with Swift 3.0, you may receive a prompt saying "Convert to Current Swift Syntax?" when opening your project in Xcode 8 (following the installation of BMSCore) do not convert BMSPush, BMSCore or BMSAnalyticsAPI

This will installs your dependencies and creates a new Xcode workspace.
***Note:*** Ensure that you always open the new Xcode workspace, instead of the original Xcode project file:

```
MyApp.xcworkspace
```

### Carthage
To install BMSPush using Carthage, add it to your Cartfile:

```
github "ibm-bluemix-mobile-services/bms-clientsdk-swift-push"
```

Then run the `carthage update` command. Once the build is finished, drag `BMSPush.framework`,`BMSCore.framework` and `BMSAnalyticsAPI.framework` into your Xcode project.

To complete the integration, follow the instructions [here](https://github.com/Carthage/Carthage#getting-started).

#### Xcode 8

For apps built with Swift 2.3, use the command `carthage update --toolchain com.apple.dt.toolchain.Swift_2_3.` Otherwise, use `carthage update`

## Enabling iOS applications to receive push notifications

### Reference the SDK in your code.

```
import BMSPush
import BMSCore
```
### Initializing the Core SDK

```
let myBMSClient = BMSClient.sharedInstance

//Swift3

myBMSClient.initialize(bluemixRegion: "Location where your app Hosted")

//Swift 2.3 or Older

myBMSClient.initialize(bluemixRegion: "Location where your app Hosted")

```

##### bluemixRegion

- Specifies the location where the app hosted. You can either use one of three values - `BMSClient.Region.usSouth`, `BMSClient.Region.unitedKingdom`, `BMSClient.Region.germany` and `BMSClient.Region.sydney` OR specify the region manually .

>**Note**:  If you are using dedicated service please use `overrideServerHost` and add `bluemixRegion` any value.

### Initializing the Push SDK

 initialize the `BMSPushClient`  using the following code.
```
let push =  BMSPushClient.sharedInstance

//Swift 3

push.initializeWithAppGUID(appGUID: "your push appGUID", clientSecret:"your push client secret")

//Swift Older

push.initializeWithAppGUID(appGUID:"your push appGUID", clientSecret:"your push client secret")

```

##### appGUID

- The Push app GUID value.

##### clientSecret

- The Push client secret value.

>**Note**: If you are using Xcode8 beta, add `yourApp.entitlements`. To do this, go to Targets -> Capabilities and enable Push Notifications capability.

### BMSPushObserver for initialize callback

 To get the `initializeWithAppGUID(..)` callback , use the following;

 1. Add the `BMSPushObserver` `protocol` in your AppDelegate

    ```
     class AppDelegate: UIResponder, UIApplicationDelegate, BMSPushObserver
    ```
 2. Set the delegate for  `BMSPushObserver`

    ```
    let push =  BMSPushClient.sharedInstance
    push.delegate = self
    ```
 3. Implement the `BMSPushObserver` function

   ```
   func onChangePermission(status: Bool) {
     print("Push Notification is enabled:  \(status)" as NSString)
    }
   ```

### Registering iOS applications and devices with userId

For `userId` based notification, the register method will accept one more parameter - `userId`

```
//Swift3

func application (_ application: UIApplication, didRegisterForRemoteNotificationsWithDeviceToken deviceToken: Data){

   let push =  BMSPushClient.sharedInstance
   push.registerWithDeviceToken(deviceToken: deviceToken, WithUserId: "your userId") { (response, statusCode, error) -> Void in
    if error.isEmpty {
      print( "Response during device registration : \(response)")
      print( "status code during device registration : \(statusCode)")
    } else{
      print( "Error during device registration \(error) ")
      Print( "Error during device registration \n  - status code: \(statusCode) \n Error :\(error) \n")
    }
}

//Swift2.3 and Older

func application (application: UIApplication, didRegisterForRemoteNotificationsWithDeviceToken deviceToken: NSData){

    let push =  BMSPushClient.sharedInstance
    push.registerWithDeviceToken(deviceToken, WithUserId: "your userId") { (response, statusCode, error) -> Void in
        if error.isEmpty {
            print( "Response during device registration : \(response)")
            print( "status code during device registration : \(statusCode)")
        }else{
            print( "Error during device registration \(error) ")
            Print( "Error during device registration \n  - status code: \(statusCode) \n Error :\(error) \n")
        }
    }
}
```

##### WithUserId

- The User Id value you want to register in the push service

>**Note**: If userId is provided the client secret value must be provided.

### Retrieve Available Tags and subscribe for Tags based Notifications

##### Retrieve Available tags

The `retrieveAvailableTagsWithCompletionHandler` API returns the list of available tags to which the device
can subscribe. After the device is subscribed to a particular tag, the device can receive any push notifications
that are sent for that tag.Call the push service to get subscriptions for a tag.

Copy the following code snippets into your Swift mobile application to get a list of available tags to which the
device can subscribe.

```

//Swift3

push.retrieveAvailableTagsWithCompletionHandler(completionHandler: { (response, statusCode, error) -> Void in

  if error.isEmpty {
    print( "Response during retrieve tags : \(response)")
    print( "status code during retrieve tags : \(statusCode)")
  }else{
    print( "Error during retrieve tags \(error) ")
    Print( "Error during retrieve tags \n  - status code: \(statusCode) \n Error :\(error) \n")
  }
}

//Swift2.3 and Older

push.retrieveAvailableTagsWithCompletionHandler({ (response, statusCode, error) -> Void in

    if error.isEmpty {
        print( "Response during retrieve tags : \(response)")
        print( "status code during retrieve tags : \(statusCode)")
    }else{
        print( "Error during retrieve tags \(error) ")
        Print( "Error during retrieve tags \n  - status code: \(statusCode) \n Error :\(error) \n")
    }
}
```
##### Subscribe to Available tags

```

//Swift3

 push.subscribeToTags(tagsArray: response!, completionHandler: { (response, statusCode, error) -> Void in

   if error.isEmpty {
       print( "Response during Subscribing to tags : \(response?.description)")
       print( "status code during Subscribing tags : \(statusCode)")
     }else{
       print( "Error during subscribing tags \(error) ")
       Print( "Error during subscribing tags \n  - status code: \(statusCode) \n Error :\(error) \n")
     }
 }

//Swift2.3 and Older

push.subscribeToTags(response, completionHandler: { (response, statusCode, error) -> Void in

    if error.isEmpty {
        print( "Response during Subscribing to tags : \(response?.description)")
        print( "status code during Subscribing tags : \(statusCode)")
    }else {
        print( "Error during subscribing tags \(error) ")
        Print( "Error during subscribing tags \n  - status code: \(statusCode) \n Error :\(error) \n")
    }
}
```

##### Retrieve Subscribed tags

```

//Swift3
 push.retrieveSubscriptionsWithCompletionHandler(completionHandler: { (response, statusCode, error) -> Void in

   if error.isEmpty {
     print( "Response during retrieving subscribed tags : \(response?.description)")
     print( "status code during retrieving subscribed tags : \(statusCode)")
   }else{
     print( "Error during retrieving subscribed tags \(error) ")
     Print( "Error during retrieving subscribed tags \n  - status code: \(statusCode) \n Error :\(error) \n")
   }
 }

//Swift2.3 and Older
push.retrieveSubscriptionsWithCompletionHandler { (response, statusCode, error) -> Void in

    if error.isEmpty {
        print( "Response during retrieving subscribed tags : \(response?.description)")
        print( "status code during retrieving subscribed tags : \(statusCode)")
    }else {
        print( "Error during retrieving subscribed tags \(error) ")
        Print( "Error during retrieving subscribed tags \n  - status code: \(statusCode) \n Error :\(error) \n")
    }
}
```
### Unsubscribing from tags based notifications

Use the following code snippets to allow your devices to get unsubscribe
from a tag.

```

//Swift3
push.unsubscribeFromTags(tagsArray: response!, completionHandler: { (response, statusCode, error) -> Void in

  if error.isEmpty {
    print( "Response during unsubscribed tags : \(response?.description)")
    print( "status code during unsubscribed tags : \(statusCode)")
  }else{
    print( "Error during  unsubscribed tags \(error) ")
  }
}

//Swift2.3 and Older

push.unsubscribeFromTags(response, completionHandler: { (response, statusCode, error) -> Void in

    if error.isEmpty {

        print( "Response during unsubscribed tags : \(response?.description)")

        print( "status code during unsubscribed tags : \(statusCode)")
    }
    else {
        print( "Error during  unsubscribed tags \(error) ")

        print( "Error during unsubscribed tags \n  - status code: \(statusCode) \n Error :\(error) \n")
    }
}
```
### Unregistering the Device from Bluemix Push Notification

Use the following code snippets to Unregister the device from Bluemix Push Notification

```

//Swift3

push.unregisterDevice(completionHandler: { (response, statusCode, error) -> Void in

  if error.isEmpty {
     print( "Response during unregistering device : \(response)")
     print( "status code during unregistering device : \(statusCode)")
   }else{
     print( "Error during unregistering device \(error) ")
   }
}

//Swift2.3 and Older

push.unregisterDevice({ (response, statusCode, error) -> Void in

    if error.isEmpty {
        print( "Response during unregistering device : \(response)")
        print( "status code during unregistering device : \(statusCode)")
    }else{
        print( "Error during unregistering device \(error) ")
        print( "Error during unregistering device \n  - status code: \(statusCode) \n Error :\(error) \n")
    }
}
```

### Enabling interactive push notifications

To enable interactive push notifications, the notification action parameters must be passed in as part of the notification object.  The following is a sample code to enable interactive notifications.

```
let actionOne = BMSPushNotificationAction(identifierName: "FIRST", buttonTitle: "Accept", isAuthenticationRequired: false, defineActivationMode: UIUserNotificationActivationMode.background)

let actionTwo = BMSPushNotificationAction(identifierName: "SECOND", buttonTitle: "Reject", isAuthenticationRequired: false, defineActivationMode: UIUserNotificationActivationMode.background)

let category = BMSPushNotificationActionCategory(identifierName: "category", buttonActions: [actionOne, actionTwo])

let notificationOptions = BMSPushClientOptions()
notifOptions.setInteractiveNotificationCategories(categoryName: [category])

let push = BMSPushClient.sharedInstance.initializeWithAppGUID(appGUID: "APP-GUID-HERE", clientSecret:"CLIENT-SECRET-HERE", options: notificationOptions)

```

### Enabling Rich Push notification support in iOS 10 (Audio, Video, GIF and Images)

To receive rich push notifications with iOS10, implement ```UNNotificationServiceExtension```.  The extension will intercept the rich push notification and it needs to be handled here.  While sending the notification from the server, all the four fields, alert, title, subtitle, attachmentURL must be specified.

In the didReceive() method of your service extension, add the following code to retrieve the rich notification content.

```
override func didReceive(_ request: UNNotificationRequest, withContentHandler contentHandler: @escaping (UNNotificationContent) -> Void) {
       self.contentHandler = contentHandler
        bestAttemptContent = (request.content.mutableCopy() as? UNMutableNotificationContent)

        BMSPushRichPushNotificationOptions.didReceive(request, withContentHandler: contentHandler)
        }
```

## Enable Monitoring.

To see the push notification monitoring status for iOS you have add the following code snippets.

Swift 3
```
// Send notification status when app is opened by clicking the notifications
func application(_ application: UIApplication, didReceiveRemoteNotification userInfo: [AnyHashable : Any]) {

     let push =  BMSPushClient.sharedInstance
     let respJson = (userInfo as NSDictionary).value(forKey: "payload") as! String
     let data = respJson.data(using: String.Encoding.utf8)

     let jsonResponse:NSDictionary = try! JSONSerialization.jsonObject(with: data! , options: JSONSerialization.ReadingOptions.allowFragments) as! NSDictionary

     let messageId:String = jsonResponse.value(forKey: "nid") as! String
     push.sendMessageDeliveryStatus(messageId: messageId) { (res, ss, ee) in
         print("Send message status to the Push server")
     }
}

// Send notification status when the app is in background mode.
func application(_ application: UIApplication, didReceiveRemoteNotification userInfo: [AnyHashable : Any], fetchCompletionHandler completionHandler: @escaping (UIBackgroundFetchResult) -> Void) {

   let payLoad = ((((userInfo as NSDictionary).value(forKey: "aps") as! NSDictionary).value(forKey: "alert") as! NSDictionary).value(forKey: "body") as! NSString)

   self.showAlert(title: "Recieved Push notifications", message: payLoad)

   let push =  BMSPushClient.sharedInstance

   let respJson = (userInfo as NSDictionary).value(forKey: "payload") as! String
   let data = respJson.data(using: String.Encoding.utf8)

   let jsonResponse:NSDictionary = try! JSONSerialization.jsonObject(with: data! , options: JSONSerialization.ReadingOptions.allowFragments) as! NSDictionary

   let messageId:String = jsonResponse.value(forKey: "nid") as! String
   push.sendMessageDeliveryStatus(messageId: messageId) { (res, ss, ee) in
       completionHandler(UIBackgroundFetchResult.newData)
   }
}
```
Swift 2.3

```
func application(application: UIApplication, didReceiveRemoteNotification userInfo: [NSObject : AnyObject]) {

  let respJson = (userInfo as NSDictionary).valueForKey("payload") as! String
  let data = respJson.dataUsingEncoding(NSUTF8StringEncoding)

  do {
      let responseObject:NSDictionary = try NSJSONSerialization.JSONObjectWithData(data!, options: []) as! NSDictionary
      let nid = responseObject.valueForKey("nid") as! String
      print(nid)

      let push =  BMSPushClient.sharedInstance

      push.sendMessageDeliveryStatus(nid, completionHandler: { (response, statusCode, error) in

          print("Send message status to the Push server")
      })

  } catch let error as NSError {
      print("error: \(error.localizedDescription)")
  }
}

func application(application: UIApplication, didReceiveRemoteNotification userInfo: [NSObject : AnyObject], fetchCompletionHandler completionHandler: (UIBackgroundFetchResult) -> Void) {

  let payLoad = ((((userInfo as NSDictionary).valueForKey("aps") as! NSDictionary).valueForKey("alert") as! NSDictionary).valueForKey("body") as! NSString)

  self.showAlert("Recieved Push notifications", message: payLoad)

  let respJson = (userInfo as NSDictionary).valueForKey("payload") as! String
  let data = respJson.dataUsingEncoding(NSUTF8StringEncoding)

  do {
      let responseObject:NSDictionary = try NSJSONSerialization.JSONObjectWithData(data!, options: []) as! NSDictionary
      let nid = responseObject.valueForKey("nid") as! String
      print(nid)

      let push =  BMSPushClient.sharedInstance

      push.sendMessageDeliveryStatus(nid, completionHandler: { (response, statusCode, error) in
          completionHandler(UIBackgroundFetchResult.NewData)
      })

  } catch let error as NSError {
      print("error: \(error.localizedDescription)")
  }
}
```
>**Note**: To get the message status when the app is in background you have to send either MIXED or SILENT push notifications. If the app is force quite you will not get any message delivery status.

### Open Url by clicking push notifications.

To open a url by clicking the push notification you can send a `url` firld inside the payload.
```
{
  "message": {
    "alert": "Notification alert message",
    "url":"https://console.ng.bliuemix.net"
  }
}
```

In your applications, go to `AppDelegate` file and inside `didFinishLaunchingWithOptions` check the value for `url`

```
let remoteNotif = launchOptions?[UIApplicationLaunchOptionsKey.remoteNotification] as? NSDictionary

if remoteNotif != nil {
    let urlField = (remoteNotif?.value(forKey: "url") as! String)
    application.open(URL(string: urlField)!, options: [:], completionHandler: nil)
}
```

### Adding custom DeviceId for registration

To send `DeviceId` please use `BMSPushClientOptions` class method,

```
let notifOptions = BMSPushClientOptions()
notifOptions.setDeviceId(deviceId: "YOUR_DEVICE_ID")
```
>**Note**: Remember to keep custom DeviceId unique for each device.

### Samples & videos

* Please visit for samples - [Github Sample](https://github.com/ibm-bluemix-mobile-services/bms-samples-swift-hellopush)

* Video Tutorials Available here - [Bluemix Push Notifications](https://www.youtube.com/channel/UCRr2Wou-z91fD6QOYtZiHGA)

### Learning More

* Visit the **[Bluemix Developers Community](https://developer.ibm.com/bluemix/)**.

* [Getting started with IBM MobileFirst Platform for iOS](https://www.ng.bluemix.net/docs/mobile/index.html)

### Connect with Bluemix

[Twitter](https://twitter.com/ibmbluemix) |
[YouTube](https://www.youtube.com/playlist?list=PLzpeuWUENMK2d3L5qCITo2GQEt-7r0oqm) |
[Blog](https://developer.ibm.com/bluemix/blog/) |
[Facebook](https://www.facebook.com/ibmbluemix) |
[Meetup](http://www.meetup.com/bluemix/)

=======================
Copyright 2016 IBM Corp.

Licensed under the Apache License, Version 2.0 (the "License");
you may not use this file except in compliance with the License.
You may obtain a copy of the License at

http://www.apache.org/licenses/LICENSE-2.0

Unless required by applicable law or agreed to in writing, software
distributed under the License is distributed on an "AS IS" BASIS,
WITHOUT WARRANTIES OR CONDITIONS OF ANY KIND, either express or implied.
See the License for the specific language governing permissions and
limitations under the License.

redpajama_set_name: RedPajamaGithub


Gathering information about your child's cancer or blood disorder diagnosis is often helpful. Your doctors, social workers, and this website provides materials that may help while your child undergoes cancer or blood disorder treatment. The health care providers are your best resource. Other good sources of information are books and pamphlets. Your social worker can guide you to these reading materials.
Why is a stem cell transplant necessary?


text:
A Beginner's Guide to Smart Contracts
''Smart' contracts will have a disruptive effect on traditional contractual performance, both practically and conceptually. However, are smart contracts actually "contracts" and are they really "smart"?
What are smart contracts?
Smart contracts are computer protocols, not contracts in the strict legal sense. They execute commercial transactions or enforce legal agreements in a manner that eliminates the need for intermediaries and their associated transaction costs.
Smart contracts represent a progression of blockchain technology from a financial transaction protocol (e.g. bitcoin) to a multi-purpose mechanism to effect business activities involving purchases and exchanges of virtually any goods, services or rights.
Smart contracts can be stored on a blockchain, interact with external data feeds and then self-execute payments, shipments of products or other actions based on conditional logic (programmed as traditional "if-then" statements – if A occurs, then B happens), agreed verifiable proof of performance, or other trigger events. In computer code, this looks something like:
function payOut(address _recipient, uint _amount) returns (bool) {
if (msg.sender != owner || msg.value > 0 || (payOwnerOnly && _recipient != owner))
throw;
if (_recipient.call.value(_amount)()) {
PayOut(_recipient, _amount);
How is a smart contract different from making purchases on the internet or setting up an automatic payment for utility bills? Generally, when you sign up online for a website you are usually directed to terms and conditions that you click to accept. Those terms and conditions are a human-readable contract. It is the same contract as you could get in hard copy just in electronic form. Laws such as the Federal Law No.1 of 2006 on Electronic Commerce and Transactions give that contract effect even though it is in electronic form.
By contrast, with a smart contract there is nothing (in theory at least) but a digital agreement. Everything from the forming of the agreement all the way to its completion happens digitally.
What the smart contract can do
Trade clearing and settlement
Manage approval workflows between counterparties, calculate trade settlement amounts, and transfer funds automatically.
Provide transfer and/or access to medical health records upon multi-signature approvals between patients and providers.
Technology, media and telecom
Royalty distribution
Calculate and distribute royalty payments to artists and other associated parties according to the contract.
Cross-industry
Peer-to-peer transacting
Match parties and transfer payments automatically for various peer-to-peer applications such as lending, insurance, energy credits, etc.
What are the potential uses of smart contracts?
Ethereum, which is a decentralized computing platform and operating system that is built specifically for creating and executing smart contracts for the "Ether" cryptocurrency using blockchain technology, is a notable smart contract application.
However, potential uses of smart contracts extend way beyond the movement of digital currency. Smart contracts could potentially be used to create peer-to-peer versions of any business model that currently involves intermediaries who handle processing and payments for a fee (e.g. banks, security exchanges, Uber or Airbnb).
By way of example, some potential uses for smart contracts across industry sectors are described in the table below:
Smart contracts and the law
"The first thing we do, let's kill all the lawyers" (William Shakespeare "Henry VI", Part II, Act IV, Scene II, Line 73)
As smart contracts are automatically enforced, smart contract enthusiasts assert that this removes the need for contract law as there is no longer any uncertainty in a smart contract transaction. From a legal perspective, smart contracts may not be that simple.
In the UAE, Article 12 of Federal Law No.1 of 2006 on Electronic Commerce and Transactions allows "smart contracts" as it provides that valid and enforceable contracts can be formed by computer programs (defined as "automated electronic agents") that include two or more electronic information systems preset and pre-programmed to carry out the transaction, even if no individual is directly involved.
The law of contract has various requirements for a contract to be valid and enforceable. For example, you cannot make an illegal contract. In the UAE a contract for gambling is illegal. You cannot have a contract to kill a person. No court will enforce such contracts.
By contrast, a smart contract is a set of instructions written in computer code that self-executes. A smart contract will do exactly what the code dictates, however ludicrous (a smart contract is not necessarily smart).
There are situations where computers cannot render contracts effectively. By way of example, written contracts frequently use wording that a party will use "reasonable endeavours". What does that mean and how do you write that in computer code?
Other fundamental legal concepts such as "good faith" and "negligence" are also very difficult to encode. These concepts are used to give the contracting parties flexibility in respect of certain obligations by not specifically determining in advance exactly what those obligations entail.
When parties agree a traditional contract, if circumstances subsequently change, there is the possibility of varying that contract. Unless the parties build into a smart contract, at the beginning, code that allows for modifications, a smart contract is not smart enough to allow for variations.
Currently, if the meaning of a contract is disputed, a court will consider what that agreement would mean to an objective and reasonable human observer. There is no such thing as a reasonable computer. Computers do not apply common sense because they are not programmed to do so.
Despite their name, smart contracts are necessarily always strictly legal contracts. At a minimum a legal contract must include the elements of offer, acceptance and the intention of the parties to enter into a legal agreement.
To the extent that legal relationships can be reduced neatly into code – so that terms are automatically enforced once the pre-programmed conditions are satisfied – smart contract technology represents an unstoppable disruptive force.
At this point in time, it seems likely that there will be a continuum between smart contracts and traditional contracts depending on the underlying transaction. A very simple contract can be fully automated (the contract is entirely in smart contract code that is stored, verified and executed on a block chain.) However more complex "smart" contracts may require a combination of both self-executing terms and contractual terms that are outside the software code. This is because:
the subject of the contract may not be readily distilled into a logic statement; and
human judgment may still be needed to determine how aspects of the contract are to be performed.
In the future, natural language computing and artificial intelligence may also overcome these barriers as well.
What is clear now is that smart contracts will revolutionise agreement making and performance of transactions.
Andrew Fawcett is a Senior Counsel in Al Tamimi & Company's Technology, Media & Telecommunications team and regularly advises on legal issues to do with blockchains.
How Does Bahrain's New Personal Data Protection Law Impact Patient Privacy?
The Federal Law regulating the Use of Information and Communication Technology in the UAE Healthcare Sector
Just Scoot over here: E-scooter Regulation in the UAE
A Space Odyssey: Licensing Satellite Based Telecommunications Services in Saudi Arabia


text:
Q: To pass 2D Dimensional array as an argument? When I run the below code , with data array as an local variable it was working fine. but, when I declared it as Global variable it was not working. can anybody please help me how to pass 2D dimensional array into the function.

  <select id="Ultra" name="letters" onchange="myFunction()">
          <option value="0">1</option>
          <option value="1">2</option>
          <option value="2">3</option>
          <option value="3">4</option>
      </select>

A: This is how to pass in a 2d array to a function. This is about as simple as I can make it. There's no need to define the type (i.e. don't do data[][]) when defining the function (I think that's where you were going wrong).
// define 2d array
var data = [[0,1],[1,3],[2,6]];

// define function
function myFunction(foobar){
    // ... do something with 2d array "foobar" ...
}

// invoke function, passing in 2d array
myFunction(data);

Example: Try it out using a tool like jsbin!

A: You can just pass the variable directly. It will still be a 2D array inside the function:
function myFunction(array) {
    // code
}

myFunction([[1,2],[3,4]]);

redpajama_set_name: RedPajamaStackExchange


text:
Q: Python: Efficient way of plotting a Gausian KDE over (x,y,z) data I have a value, z, at position, [x,y], and I would like to smooth this plot using a Gaussian KDE. The reason for this is that I would like to create "hotspots" to find the probability of an object being in a similar place.
x,y and z are 1D arrays. X and Y are irregularly spaced.
Scikit KDE's that I've looked at require that each X/Y pair be evenly weighted but I would like to weight it by Z.
I've tried matplotlib's tricontourf(x,y,z) and tripcolor(x,y,z) but the smoothing isn't what I require.


Here is a real nice folding ladies fan from the 75th anniversary of the Battle of Gettysburg. Given out during the large encampment. This is the confederate one which depicts Picket's Charge on the front with great detail. The back has maps of the three days battle. As you can see it folds and does have a few crease marks ,a couple of bends and a minor small tearr or two.
Over all a really cool piece in remarkably great condition. Comes with the ryker case you see it in. Got this from the horse Soldier back in 1996.
Please E-mail me with your order.
"Pay securely with your credit card at Paypal, without an account "
"Add to Cart to purchase "
Very attractive fully cases 1/6th ambrotype(on glass)plate of a cavalry sergeant. Plate size is 2-3/4 x 3-1/4. The case is a union "patent" gutta percha, thermoplastic case in very good condition. Made by A. P. Critchlow. & Co. The interior has the decorative felt lining on the left side, with the photo framed in a nice gold colored frame.
The photo iteslf is in good condition and shows a stern looking cavalry sergeant in a sitting pose leaning on the table. Has his saber in front of him, and wearing his gauntlets. His hat is to the left of him on a table. The buttons and stripes look painted on.
But the best part is on the back which shows a lock of hair????? been there a long time, and is very cool. There appears to be period writing on the makers insert, which as far as i can tell reads,"Jan 20 -May ? M. EW""Sat Aug-7- 1859".
I got this about 20 years ago from a local collector( i should have bought more)this has never been on the market before.


Before we see How to prophesy accurately: 13 Keys to Receive and Release a Prophetic Word, I want us to first of all understand what is prophecy and how the prophets of old or old testament believers received prophetic utterances. I trust this teaching will launch you into a deeper phase in the prophetic. You will learn how to receive and release prophetic utterances effectively. This kind of teaching can only be found on Voice of Dominion; so, don't forget to subscribe for more in dept teachings.
A prophecy is a message inspired by God, a divine revelation. The Bible says that prophets "spoke from God as they were moved by holy spirit." (2 Peter 1: 20, 21) So a prophet is one who receives God's message and transmits it to others. —Acts 3: 18.
How did prophets receive information from God?
Writing. God used this method in at least one case by directly supplying to Moses the Ten Commandments in written form. —Exodus 31:18.
Visions. These were sometimes given while the prophet was awake and fully conscious. (Isaiah 1:1; Habakkuk 1:1) Some were so vivid that the recipient participated in them. (Luke 9: 28- 36; Revelation 1: 10- 17) At other times, visions were conveyed while the recipient was in a trance. (Acts 10:10, 11; 22:17- 21) God also transmitted his message by dreams while the prophet slept. —Daniel 7:1; Acts 16: 9, 10.
Mental guidance. God guided the thoughts of his prophets to convey his message. This is the sense of the Bible's statement: "All Scripture is inspired of God." The phrase "inspired of God" can also be rendered "God-breathed." (2 Timothy 3: 16; The Emphasised Bible) God used his holy spirit, or active force, to "breathe" his ideas into the minds of his servants. The message was God's, but the prophet selected the wording. —2 Samuel 23: 1, 2.
No, Bible prophecy is not limited to foretelling the future. However, most messages from God relate to the future, even if only indirectly. For example, God's prophets repeatedly warned the ancient Israelites about their evil ways. Those warnings described the future blessings if the people would heed the warning, as well as the future calamity if they refused. (Jeremiah 25: 4-6) The actual outcome depended on the course that the Israelites chose to follow. —Deuteronomy 30:19, 20.
On one occasion when the Israelites asked God for help, he sent a prophet to explain that because they had refused to obey God's commands, He had not helped them. —Judges 6: 6- 10.
When Jesus spoke to a Samaritan woman, he revealed things about her past that he could have known only by divine revelation. She recognized him as a prophet even though he had made no predictions about the future. —John 4: 17- 19.
At Jesus' trial, his enemies covered his face, hit him, and then said: "Prophesy! Who is it that struck you?" They were not calling for Jesus to foretell the future but for him to identify by divine power who had hit him. —Luke 22:63, 64.
2. All of the Lord's words, no matter in what form we hear them, must be quickened and revealed by the Holy Spirit. Quicken means "adding life to ordinary words." The Greek word for quicken means "to make alive and give life by spiritual power to arouse and invigorate." The word Jesus speaks has life and vitality. Other words are just dead language. The message can come in a variety of ways—flashes of pictures, Scripture verses, sentence fragments or impressions.
9. The end result of prophecy is to find a way to put honor and glory back on mankind and restore what we lost in the garden: relationship to the Father.Everyone wants his or her crown of glory and honor. People are made for validation, celebration and appreciation.


A US federal appeals court in San Francisco has overturned a patent infringement ruling against Microsoft and ordered a lower court to retry the case against the company. Originally, the verdict found that parts of Microsoft's Internet Explorer Web browser had infringed on technology developed by privately-held firm Eolas Technologies and the University of California. Now, it has been ruled that key parts of Microsoft's defence were not properly considered.
"A spokesman for Washington state-based Microsoft said it is looking forward to presenting its case again. No date has been set for a retrial."


text:
Плезант-Валли () — тауншип в округе Моуэр, Миннесота, США. На 2000 год его население составило 308 человек.

География
По данным Бюро переписи населения США площадь тауншипа составляет 78,0 км², из которых 78,0 км² занимает суша, водоёмов нет.

Демография
По данным переписи населения 2000 года здесь находились 308 человек, 100 домохозяйств и 75 семей.  Плотность населения —  3,9 чел./км².  На территории тауншипа расположено 104 постройки со средней плотностью 1,3 построек на один квадратный километр. Расовый состав населения: 97,40 % белых и 2,60 % приходится на две или более других рас. Испанцы или латиноамериканцы любой расы составляли 0,65 % от популяции тауншипа.

Из 100 домохозяйств в 43,0 % воспитывались дети до 18 лет, в 70,0 % проживали супружеские пары, в 2,0 % проживали незамужние женщины и в 25,0 % домохозяйств проживали несемейные люди. 19,0 % домохозяйств состояли из одного человека, при том 8,0 % из — одиноких пожилых людей старше 65 лет. Средний размер домохозяйства — 3,08, а семьи — 3,67 человека.

38,3 % населения — младше 18 лет, 4,2 % — в возрасте от 18 до 24 лет, 29,5 % — от 25 до 44, 18,8 % — от 45 до 64, и 9,1 % — старше 65 лет. Средний возраст — 32 года. На каждые 100 женщин приходилось 100,0 мужчин.  На каждые 100 женщин старше 18 приходилось 106,5 мужчин.

Средний годовой доход домохозяйства составлял 46 250 долларов, а средний годовой доход семьи —  48 750 долларов. Средний доход мужчин —  35 865  долларов, в то время как у женщин — 20 313. Доход на душу населения составил 14 242 доллара. За чертой бедности находились 2,6 % семей и 3,0 % всего населения тауншипа, из которых 4,3 % младше 18 лет.

Примечания

Тауншипы округа Мауэр

redpajama_set_name: RedPajamaWikipedia


In order to try & keep up with the demand for our little Daycare Swaggies we are currently making some changes behind the scenes. We will be reopening in June 2019 with two new prints. For more updates follow us on instagram @swaggies_au Thank you for all of your support!


Very welcoming staff memeber Monica is very helpful and really nice, the breakfast staff were all good too. The whole place is excellent and I would have no compunction in recommending this hotel to anyone. We wil certainly be back.
We stayed here 11th to 14th June. Everything about the hotel was very good. The staff were friendly and very efficient and nothing was too much bother for them. Our room had a wet room, I have always wanted one and was very taken with it. Breakfasts were tailor made to your requirements. The weather was awful but the hotel was excellent in all respects.
We spent 3 nights in Brighton, and stayed in a superior double at Kempfield House. There was a complimentary bottle of wine, nuts, chocolates, water and coke, with a hospitality tray, a very comfortable 4 poster bed, and a huge bath. The room was a good size, and we had plenty of room even with a travel cot set up for my son. All thr staff were lovely & very friendly, all of them interacted with our son which made us feel even more welcome. Breakfast was delicious, with good quality and local food. The hotel is in a prime location, near to the pier, the laines and all other attractions, but is still quiet at night. I would thoroughly recommend Kemofield House to anybody looking to stay in Brighton.
Excellent place to stay in a couldnt be better location. Room a really decent size, good bathroom which was a wet room - not to everyones taste but was fine. Really appreciated the fridge in the room and the complimentary refreshments. One tiny point - the room we were in had a metal framed bed which was extremely squeaky, and to be honest, a bit annoying. but other than that - fab place. thanks.
Me and my girlfriend couldn't of been happier with every aspect of our stay. I have recommended that my colleagues and friends stay here when in Brighton.
Thanks to Chris and especially Scarlett, both were incredibly helpful.
The only B&B in Brighton i would consider returning to. I had an excellent stay and the breakfast was delightful and pleasantly delivered.
Lovely hotel, friendly staff and comfortable double room. Breakfast catered for specific dietary requirements and the friendly waiting staff remembered them the following day without being asked. Would definitely stay again!
We arrived very early and left our luggage. The young lady at the reception took our number and was able to contact us very soon to tell us they had a room ready for us ahead of time. Breakfast staff was very friendly and helpful as well. Comfortable room and good location.


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