text:
package eu.ehealth.controllers;

import java.util.ArrayList;
import java.util.Collection;
import org.zkoss.zk.ui.Component;
import org.zkoss.zk.ui.Executions;
import org.zkoss.zk.ui.Session;
import org.zkoss.zk.ui.Sessions;
import org.zkoss.zk.ui.event.Event;
import org.zkoss.zk.ui.event.EventListener;
import org.zkoss.util.resource.Labels;
import org.zkoss.zul.Button;
import org.zkoss.zul.Grid;
import org.zkoss.zul.Hbox;
import org.zkoss.zul.Include;
import org.zkoss.zul.Label;
import org.zkoss.zul.Messagebox;
import org.zkoss.zul.Row;
import org.zkoss.zul.Rows;
import org.zkoss.zul.Textbox;
import org.zkoss.zul.Window;
import eu.ehealth.SystemDictionary;
import eu.ehealth.utilities.ComponentsFinder;
import eu.ehealth.ws_client.StorageComponentImpl;
import eu.ehealth.ws_client.xsd.Carer;
import eu.ehealth.ws_client.xsd.Clinician;
import eu.ehealth.ws_client.xsd.Consulter;
import eu.ehealth.ws_client.xsd.GeneralPractitioner;
import eu.ehealth.ws_client.xsd.OperationResult;
import eu.ehealth.ws_client.xsd.Patient;
import eu.ehealth.ws_client.xsd.PersonData;
import eu.ehealth.ws_client.xsd.SocialWorker;
import eu.ehealth.ws_client.xsd.SocioDemographicData;
import eu.ehealth.ws_client.xsd.User;

/**
 * This class handles the creation and the events of the Patient questionnaire.
 *
 * @author Xavi Sarda (Atos Origin)
 */
public class PattientControllerWindow extends SDFormControllerWindow
{

	private static final long serialVersionUID = 3014122995824061686L;
	private CarerListWindowController clist = null;
	private String currentresp = null;
	private SocialWorker currentsocialworker = null;
	private Consulter currentconsulter = null;
	private GeneralPractitioner currentgeneralpracticioner = null;
	private Carer currentcarers = null;

	/**
	 * Default constructor
	 */
	public PattientControllerWindow()
	{
		isNewUser = true;
		this.buildForm(true);
	}

	/**
	 * Constructor to change the create form into an update form
	 *
	 * @param current Patient to be updated
	 */
	public PattientControllerWindow(Patient current)
	{
		isNewUser = false;

		this.currentid = current.getID();
		this.currentdata = current.getPersonData();
		this.currentsd = current.getSDData();
		this.currentresp = current.getResponsibleClinicianID();
		this.currentsocialworker = current.getSocialWorker();
		this.currentconsulter = current.getConsulterInCharge();
		this.currentgeneralpracticioner = current.getGeneralPractitioner();
		this.currentcarers = current.getPatientCarer();

		this.buildForm(false);

		this.addPersonFieldsValues();
		this.addAddressFieldsValues();
		this.addCommunicationFieldsValues();
		this.addSocioDemographicDataFieldsValue();
		this.addResponsibleClinicianFieldValues();
		this.addCarerFieldValues();
		this.addSocialWorkerConsulterAndGPFieldsValues();
		this.appendChild(this.createUpdateButton());
		this.getFellow("pat_uname").getParent().setVisible(false);
	}

	/**
	 * Build form instructions to be executed
	 */
	public void buildForm(boolean newPatient)
	{
		this.addErrorBox();
		this.addResponsibleClinicianField();
		this.addPersonFields(newPatient);
		this.addAddressFields();
		this.addCommunicationFields();
		this.addSocioDemographicDataFields();
		this.addCarerField();
		this.addSocialWorkerConsulterAndGPFields();
	}

	/**
	 * Submit function: Used on the view layer to create a new Patient (using
	 * the StorageComponentImpl).
	 *
	 * @return void but saves a new Patient on the server
	 */
	public void sendPatient(boolean newpatient)
	{
		if (!validateForm())
		{
			return;
		}

		OperationResult result = null;
		String resClinic = ((Textbox) getFellow("pat_respo")).getValue();
		String carerId = ((Textbox) getFellow("pat_carid")).getValue();

		// Getting information from form fields
		SocioDemographicData sdData = this.getSocioDemographicData();
		PersonData personData = this.getPersonData();
		SocialWorker socialw = this.getSocialWorkerData();
		Consulter consulter = this.getConsulterData();
		GeneralPractitioner gralprac = this.getGeneralPracticionerData();
		try
		{
			StorageComponentImpl proxy = SystemDictionary.getSCProxy();
			Session ses = Sessions.getCurrent();
			String id = (String) ses.getAttribute("userid");

			Carer car2set = proxy.getCarer(carerId, id);
			Patient patient = new Patient("", personData, sdData, resClinic, socialw, consulter, gralprac, car2set);

			if (newpatient)
			{
				result = proxy.createPatient(patient, id);
				String username = this.getUsername();

				User user = createNewUser(SystemDictionary.USERTYPE_PATIENT, result.getCode(), username);
				result = proxy.createUser(user);
				if (!result.getDescription().equals("ok"))
				{
					Window win = (Window) getFellow("internalformerror");
					((Label) win.getFellow("errorlbl")).setValue("Username not valid");
					getFellow("internalformerror").setVisible(true);
					proxy.deletePatient(user.getPersonID(), id);
					return;
				}

				Messagebox.show("#TXT# User (id= " + result.getCode() + ") created succesfully", "#TXT# Create New User",
						Messagebox.OK, Messagebox.INFORMATION);
			}
			else
			{
				patient.setID(this.currentid);
				result = proxy.updatePatient(patient, id);

				Messagebox.show("#TXT# User modified succesfully", "#TXT# Modify User", Messagebox.OK, Messagebox.INFORMATION);
			}

			Collection<Component> col = Executions.getCurrent().getDesktop().getComponents();
			Include comp = (Include) ComponentsFinder.getUIComponent(col, "app_content");
			comp.setSrc("../patients/index_content.zul");
		}
		catch (Exception e)
		{
			SystemDictionary.logException(e);
			Messagebox.show("#TXT# Error : " + e.getMessage(), "#TXT# Create New User", Messagebox.OK, Messagebox.ERROR);
		}
	}

	/**
	 * Creates a modal window to select a primary carer for the patient
	 *
	 * @throws InterruptedException
	 */
	public void createDialog() throws InterruptedException
	{
		try
		{
			this.clist = new CarerListWindowController(this);
			this.appendChild(this.clist);
			this.clist.doModal();

			this.clist = null;
		}
		catch (Exception e)
		{
			SystemDictionary.logException(e);
		}
	}

	/**
	 * This method creates a clinician list for the patient form. It is also in
	 * charge of attaching it to the form and showing it in a modal mode
	 *
	 * @throws InterruptedException
	 */
	public void createClinicianDialog() throws InterruptedException
	{
		if (this.getFellowIfAny("rclinlistwin") == null)
		{
			ClinicianListForPatients respolist =
					(ClinicianListForPatients) Executions.getCurrent().createComponents("../patients/clinlist.zul", this, null);
			respolist.doModal();
		}
	}

	/**
	 * This method is used to set Carer form fields with information from the
	 * modal dialog fields
	 *
	 * @param carerID
	 * @param carerName
	 */
	public void setCarer(String carerID, String carerName)
	{
		((Textbox) this.getFellow("pat_carid")).setValue(carerID);
		((Textbox) this.getFellow("pat_carname")).setValue(carerName);
	}

	/**
	 * This method is used to set responsible clinician form fields with
	 * information from the modal dialog fields
	 *
	 * @param clinID Id of the responsible clinician
	 * @param clinName Name of the responsible clinician
	 */
	public void setResponsibleClinician(String clinID, String clinName)
	{
		((Textbox) this.getFellow("pat_respo")).setValue(clinID);
		((Textbox) this.getFellow("pat_respo_lbl")).setValue(clinName);
	}

	/**
	 * Protected function to add a responsible clinician field to the window.
	 */
	protected void addResponsibleClinicianField()
	{
		String respo = Labels.getLabel("patients.form.responsible");

		ArrayList<SimpleFieldData> rowsA = new ArrayList<SimpleFieldData>();
		rowsA.add(new SimpleFieldData(respo, "pat_respo_lbl"));

		Grid pgrid = new Grid();
		pgrid.setSclass("grid");
		this.appendColumns(pgrid);

		Rows rows = new Rows();

		Row rowhidf = new Row();
		Label lbl_ins = new Label(respo);
		rowhidf.appendChild(lbl_ins);
		Hbox hbox1 = new Hbox();
		Textbox tbox1 = new Textbox();
		tbox1.setId("pat_respo_lbl");
		tbox1.setReadonly(true);
		tbox1.addEventListener("onClick", new EventListener() {
			public void onEvent(Event arg0) throws Exception
			{
				createClinicianDialog();
			}
		});

		Textbox tbox2 = new Textbox();
		tbox2.setVisible(false);
		tbox2.setId("pat_respo");

		hbox1.appendChild(tbox1);
		hbox1.appendChild(tbox2);
		rowhidf.appendChild(hbox1);
		rows.appendChild(rowhidf);

		pgrid.appendChild(rows);
		this.appendChild(pgrid);
	}

	/**
	 * This method sets the responsible clinician values when updating a form
	 */
	protected void addResponsibleClinicianFieldValues()
	{
		String id = (String) Sessions.getCurrent().getAttribute("userid");
		StorageComponentImpl proxy = new StorageComponentImpl();
		try
		{
			Clinician clinician = proxy.getClinician(this.currentresp, id);
			((Textbox) getFellow("pat_respo")).setValue(this.currentresp);
			((Textbox) getFellow("pat_respo_lbl")).setValue(clinician.toString());
		}
		catch (Exception re)
		{
			((Textbox) getFellow("pat_respo_lbl")).setValue("Not available");
		}
	}

	/**
	 * This method appends a carer field to the window. Button will open a modal
	 * dialog to select a carer
	 *
	 * @see CarerListWindowController
	 */
	protected void addCarerField()
	{
		String carertitle = Labels.getLabel("patients.carer.title");
		String carerlabel = Labels.getLabel("patients.carer.label");

		Grid pgrid = new Grid();
		pgrid.setSclass("grid");
		this.appendColumns(pgrid);

		Rows rows = new Rows();

		this.appendSubFormTitleRow(carertitle, rows);

		Row row = new Row();
		Label lab = new Label();
		lab.setValue(carerlabel);
		row.appendChild(lab);

		Hbox hbox01 = new Hbox();

		Textbox tbox = new Textbox();
		tbox.setId("pat_carname");
		tbox.setReadonly(true);

		Textbox tbox2 = new Textbox();
		tbox2.setId("pat_carid");
		tbox2.setVisible(false);
		tbox2.setReadonly(true);

		tbox.addEventListener("onClick", new EventListener() {
			public void onEvent(Event arg0) throws Exception
			{
				createDialog();
			}
		});

		hbox01.appendChild(tbox);
		hbox01.appendChild(tbox2);
		row.appendChild(hbox01);

		rows.appendChild(row);

		pgrid.appendChild(rows);
		this.appendChild(pgrid);
	}

	/**
	 * This method sets the carer values when updating a patient
	 */
	protected void addCarerFieldValues()
	{
		((Textbox) getFellow("pat_carid")).setValue(this.currentcarers.getID());
		((Textbox) getFellow("pat_carname")).setValue(
				this.currentcarers.getPersonData().getName() + ", " + this.currentcarers.getPersonData().getSurname());
	}

	/**
	 * This method adds the social worker, consulter and general practicioner
	 * fields in the form
	 */
	protected void addSocialWorkerConsulterAndGPFields()
	{
		Grid pgrid1 = new Grid();
		Grid pgrid2 = new Grid();
		Grid pgrid3 = new Grid();
		pgrid1.setSclass("grid");
		pgrid2.setSclass("grid");
		pgrid3.setSclass("grid");
		this.appendColumns(pgrid1);
		this.appendColumns(pgrid2);
		this.appendColumns(pgrid3);

		Rows rows1 = new Rows();
		Rows rows2 = new Rows();
		Rows rows3 = new Rows();

		this.appendSubFormTitleRow("#TXT# Social Workrer Info", rows1);
		this.appendSubFormTitleRow("#TXT# Consulter Info", rows2);
		this.appendSubFormTitleRow("#TXT# General Practicioner Info", rows3);

		ArrayList<SimpleFieldData> rowsA = new ArrayList<SimpleFieldData>();
		rowsA.add(new SimpleFieldData("#TXT# Name", "pat_swname"));
		rowsA.add(new SimpleFieldData("#TXT# E-mail", "pat_swmail"));
		rowsA.add(new SimpleFieldData("#TXT# Phone", "pat_swphone"));

		ArrayList<SimpleFieldData> rowsB = new ArrayList<SimpleFieldData>();
		rowsB.add(new SimpleFieldData("#TXT# Name", "pat_consname"));
		rowsB.add(new SimpleFieldData("#TXT# E-mail", "pat_consmail"));
		rowsB.add(new SimpleFieldData("#TXT# Phone", "pat_consphone"));

		ArrayList<SimpleFieldData> rowsC = new ArrayList<SimpleFieldData>();
		rowsC.add(new SimpleFieldData("#TXT# Name", "pat_gpname"));
		rowsC.add(new SimpleFieldData("#TXT# E-mail", "pat_gpmail"));
		rowsC.add(new SimpleFieldData("#TXT# Phone", "pat_gpphone"));

		this.appendTextboxFields(rowsA, rows1);
		this.appendTextboxFields(rowsB, rows2);
		this.appendTextboxFields(rowsC, rows3);

		pgrid1.appendChild(rows1);
		pgrid2.appendChild(rows2);
		pgrid3.appendChild(rows3);
		this.appendChild(pgrid1);
		this.appendChild(pgrid2);
		this.appendChild(pgrid3);
	}

	/**
	 * This method adds the social worker, consulter and general practicioner
	 * values when updating a patient
	 */
	protected void addSocialWorkerConsulterAndGPFieldsValues()
	{
		((Textbox) getFellow("pat_swname")).setValue(this.currentsocialworker.getName());
		((Textbox) getFellow("pat_swmail")).setValue(this.currentsocialworker.getEmail());
		((Textbox) getFellow("pat_swphone")).setValue(this.currentsocialworker.getPhone());

		((Textbox) getFellow("pat_consname")).setValue(this.currentconsulter.getName());
		((Textbox) getFellow("pat_consmail")).setValue(this.currentconsulter.getEmail());
		((Textbox) getFellow("pat_consphone")).setValue(this.currentconsulter.getPhone());

		((Textbox) getFellow("pat_gpname")).setValue(this.currentgeneralpracticioner.getName());
		((Textbox) getFellow("pat_gpmail")).setValue(this.currentgeneralpracticioner.getEmail());
		((Textbox) getFellow("pat_gpphone")).setValue(this.currentgeneralpracticioner.getPhone());
	}

	/**
	 * Method to retrieve a SocialWorker from the form
	 *
	 * @return SocialWorker defined on the patient form
	 */
	protected SocialWorker getSocialWorkerData()
	{
		String name = ((Textbox) getFellow("pat_swname")).getValue();
		String mail = ((Textbox) getFellow("pat_swmail")).getValue();
		String phone = ((Textbox) getFellow("pat_swphone")).getValue();
		return new SocialWorker(name, phone, mail);
	}

	/**
	 * Method to retrieve the consulter from the form
	 *
	 * @return Consulter defined on the patient form
	 */
	protected Consulter getConsulterData()
	{
		String name = ((Textbox) getFellow("pat_consname")).getValue();
		String mail = ((Textbox) getFellow("pat_consmail")).getValue();
		String phone = ((Textbox) getFellow("pat_consphone")).getValue();
		return new Consulter(name, phone, mail);
	}

	/**
	 * Method to retrieve a GeneralPracticioner from the form
	 *
	 * @return GeneralPracticioner defined on the patient form
	 */
	protected GeneralPractitioner getGeneralPracticionerData()
	{
		String name = ((Textbox) getFellow("pat_gpname")).getValue();
		String mail = ((Textbox) getFellow("pat_gpmail")).getValue();
		String phone = ((Textbox) getFellow("pat_gpphone")).getValue();
		return new GeneralPractitioner(name, phone, mail);
	}

	/**
	 * Method in charge of creating update button for patients updates
	 * operations
	 *
	 * @return Button to be added to the form
	 */
	public Button createUpdateButton()
	{
		Button btn = new Button();
		String text = Labels.getLabel("patients.update.title");
		btn.setLabel(text);
		btn.addEventListener("onClick", new EventListener() {
			public void onEvent(Event arg0) throws Exception
			{
				sendPatient(false);
			}
		});

		return btn;
	}

	/**
	 *
	 * @return
	 */
	private boolean validateForm() {
		try {
			// check common fields
			if (!validateFormCommonFields())
				return false;

			if (((Textbox) getFellow("pat_respo")).getValue() == null || ((Textbox) getFellow("pat_respo")).getValue().trim().equals(""))
			{
				Window win = (Window) getFellow("internalformerror");
				((Label) win.getFellow("errorlbl")).setValue("#TXT# You must select some clinician");
				getFellow("internalformerror").setVisible(true);

				return false;
			}
			else if (((Textbox) getFellow("pat_carid")).getValue() == null || ((Textbox) getFellow("pat_carid")).getValue().trim().equals(""))
			{
				Window win = (Window) getFellow("internalformerror");
				((Label) win.getFellow("errorlbl")).setValue("#TXT# You must select some carer");
				getFellow("internalformerror").setVisible(true);

				return false;
			}

			return true;
		}
		catch (Exception e)
		{
			e.printStackTrace();
			SystemDictionary.webguiLog("ERROR", e.getMessage());

			String errorMsj = e.getMessage();
			try {
				Window win = (Window) getFellow("internalformerror");
				((Label) win.getFellow("errorlbl")).setValue(errorMsj);
				getFellow("internalformerror").setVisible(true);
				((Label) win.getFellow("errorlbl")).setFocus(true);
				return false;
			}
			catch (Exception ex) {}

			return false;
		}
	}

}

redpajama_set_name: RedPajamaGithub


Want to manage companies expanding overseas?
Want to digitize trading processes?
Want to accelerate consolidated accounting?
Want to reinforce Internal Control?
Want to standardize business process flow?
Want to safely implement a system?
Supports quotation, sales orders, shipping instructions, sales, sales returns, and sales reports for merchandising businesses who handle purchases and sales of goods.
Handles purchase requests, purchase orders, purchases, purchase-related costs entry and allocation, processing orders, processing acceptance, purchase reports, purchase data transfer to Payable system, and cost calculation per purchase project.
Handles stock-in/out process, stock-in/out schedule management, reservation of car allocation, distribution arrangement, and physical inventory taking.
Specializes in service provision and handles quotations, sales orders, sales split entry, and sales reports.
We strongly recommend using this PC-POS (Point of Sale) system if you are a wholesaler using Plaza-i Sales Management (SOE) and you also sell goods in your retail stores.
This module is for system and software companies who develop and/or support software products, and information system departments of user companies.
Best suited for companies who perform cost calculation by project based on input data such as purchases by project by resource, time report, and expense report, and record sales on a construction completion basis or on a construction progress basis.
This is a module used by your accounting department who handles general ledger, trial balance, financial statements, consumption tax, and financial analysis.
Handles payable entry, payment, and A/P account management for all kinds of industry.
Handles bill closing (automatic creation of invoices), cash collection schedule management, cash collection entry, and A/R management.
Plaza-i Fixed Asset Management provides high usability as part of the ERP package system and also when used independently, and becomes compliant with tax reform in timely fashion.
Handles registration, allocation, execution, and evaluation of forward exchange contract transactions.
This module is used by staff at local offices and handles cash and bank accounts, reimbursement, and payment request processes seamlessly with the accounting system of the head office.
Handles purchase request, purchase orders, inspection, payment request, and budget management, which support workflow.
Working with Ekispart (Railway Route Search)®, this expense settlement system handles employees' travel expenses as one module of the ERP package system.
Handles salary, bonus, and social insurance calculation, year-end adjustment, payment records, and pay slip email delivery (optional function).
You can handle the progress management of the sales prospects (Sales Pipeline Management) by registering the prospects that are allocated to each sales representative and entering the statuses.
Maintains information on persons who belong to your corporate clients and also individual clients, categorizes those persons into different groups from various points of view (Selection Set) to send announcement letters, transmittal letters, New Year cards, etc., and manages transmittal history.
Data output methods can be freely defined and you can analyze data accumulated in the Plaza-i application.
This module manages master data commonly used among Plaza-i modules, such as enterprise, company, organization, client, employee, user-defined, project codes, etc.


text:
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Helayna's Senior Session, University of Pittsburgh, Oakland, PA
The Beauty of Pittsburgh...
Helayna is another gorgeous Aquinas Senior that I had the joy of photographing last Sunday morning!! I spoke with her mom, Denise on the phone a few weeks ago and we decided that Oakland, specifically the University of Pittsburgh's campus would be the best place to capture her senior photos.
The weather was not looking promising that day but I checked the radar every few minutes and we gave it a chance and I'm SO glad we did!! Helayna showed up with a huge smile and said "I love fall weather! This makes me happy!" So there were very few "giggle at the camera" moments where she didn't truly mean it!
The Beauty of a Senior...
The more seniors I capture this season, the more I fall in love with these sessions. Seniors are so vibrant and full of life. I love their sense of adventure when doing these photoshoots and this one was no different!
I will be the first to admit my sense of direction is terrible. I even went to Pitt for a year and it's been years since I've had to walk around Oakland. Thank goodness Denise works on campus as an interior designer and knows ALL the sweet spots!! Of course we started at the iconic Cathedral of Learning, right in the heart of Oakland. We walked around the grounds and Helayna and I both were mesmerized by the beautiful architecture surrounding us. How often I spent running from class to class and never took the time to really take in the beauty.
Helayna's first outfit was a dress so beautiful for fall. The natural stone reflected so beautifully on her already gorgeous face!! I know that Helayna lights up a room wherever she goes with her sparkly personality. She is smart and positive and truly fun to be around. She is such an accomplished young woman at such a young age. Helayna is so excited to attend Pitt for chemical engineering and her mom has faith that she will choose a career that will change the way we value food. I certainly hope she does!! She also excels at the cello and plays in an orchestra here in Pittsburgh. Her dedication to music and learning is something to inspire others!
The Beauty of Our Surroundings....
After we walked around the Cathedral, Helayna changed into a fabulous blue dress with a super fun hat! Not many people (aka me) can pull off the hat "look" but this girl ROCKED IT!!!! We made sure to get plenty of photos at the fountain. One of my favorites is her standing on the brim of the water (neither one of us fell in!) with the Cathedral in the background.
Some of my other favorite shots were of Helayna while playing her cello. I don't even think she realized that complete strangers stopped to listen to her beautiful music. Helayna, you have a gift and it's amazing!
Helayna is such a proud lover of Pittsburgh that I am SO excited for her to experience college life here in her hometown!! I hope we keep in touch over the years because I want to get that SAME photo of her standing in front of the University of Pittsburgh Sign four years from now, as a new college graduate. Helayna, I know your future is so promising and I can't wait to heal all about it over a butter beer latte!
(28 June, 2022)
Derek's Graduation Party, Heinz History Center, Pittsburgh, PA
Thinking Beyond the Digitals
(16 September, 2022)
Shayne's Senior Photos, Hartwood Acres
© 2023 Jennifer Kurz Photography

redpajama_set_name: RedPajamaCommonCrawl


Jo and Scott discuss what we mean by 'Christ's Kingdom' in the Riverlife vision statement, as a part of our 'Paradigm' series.
In this episode Jo and Scott interview Claudine Hawkins about 'Love Demonstrated" as the fifth episode in the paradigm series.
In this episode Jo and Scott interview Dr Lindsey Farrell about 'Love Declared" as the forth episode in the paradigm series.
Jo and Scott interview Pastor Dylan Krause about 'Empowered' as the third episode in the paradigm series.
Jo and Scott talk about 'Presence' as the second episode in the paradigm series.
Jo and Scott introduce the new series called paradigm and look at family as the first topic.
Jo and Scott catch up with Riverlife's Senior Pastor John Robertson, and discuss preparing for a move of God's presence.
In this episode Jo and Scott interview Dr Tom Jones from Global Awakening.
In this episode Jo and Scott interview Charity Cook from Global Awakening.
This is our one year anniversary episode, so lets have some fun!
In this episode Scott interviews Senior Pastor John Robertson about 'Unveiled', the vision for Riverlife for 2019.


RESIDENTS in flood-affected areas are warned to take precautions against biting insects.
The Department of Health issued the warning, with fears an increase in mosquito activity could lead to an increased risk of mosquito-borne disease.
The City of Swan is ramping up mosquito control across the region to help reduce the risk.
Swan Mayor Mick Wainwright said recent rainfall and flooding had the potential to create an unexpected boom of mosquitoes.
"The City's environmental health technical officers are currently treating standing bodies of water (such as drainage basins) that are holding unusually high levels of water and monitoring flooded areas to identify high-risk breeding areas," he said.
"Even with additional measures in place, there is still a risk of higher than normal mosquito activity over the next few weeks.
Department of Health managing scientist environmental health hazards Michael Lindsay said the wet weather and flooding had created ideal conditions for mosquito breeding.
"While local government mosquito management programs are in place around WA, it is not realistic or logistically feasible to keep mosquitoes and biting flies below nuisance levels when such vast areas of the State are affected with the recent weather conditions," Dr Lindsay said.
He said symptoms included swollen or painful joints, sore muscles, skin rashes, fever, fatigue and headaches.
"There are no specific cures or vaccines for mosquito-borne diseases in WA, so it is very important that people take care to prevent being bitten," he said.
For more information on controlling mosquitoes in your backyard visit www.swan.wa.gov.au.


Kyle S. Dorrenbacher was born in 1972 and he registered to vote, giving his address as 39471 County Road Bb, Akron, Washington County, Colorado, United States of America 80720. His voting status is: Active. He is registered in the Colorado Republican Party.


This story is from the POV of a woman looking back at her childhood in early-1960's England. It's a great portrait of an ethos, of a time when women bore shame and men did not, when children were seen and not heard, when secrets were treasured and truth wasn't very important – but concealing the truth was.
Grandmother Nana is "continually in the process of clearing out, giving things away, as if she were trying to weigh less and less, as if life itself were a mess that she was gradually getting to the bottom of." Stella "can remember being flooded with happiness once, alone in Nana's bedroom" just by feeling alive in the breeze looking at colors and textures. The fact that it was only once tells me she is not a happy child, and the fact that this does not consume her tells me that she did not expect to be a happy child. Today, she'd be bundled off to a child therapist for treatment. I probably would have been to – I was so shy in kindergarten, I walked on tiptoe and whispered when I said anything at all. It never occurred to me I could be happy. Stella and I are about the same age, and we see some things the same (my family was well-off, though the family itself was pretty much a wreck, something I didn't realize until I was much older as secrets were our strength, too).
Mum does not want to move back with Nana: "I thought of Nana as harmless, lightweight, easy to brush aside…But I knew from my mother's face that for her the idea of moving back into her old home was a living danger… The only way for her to defend herself against Nana's bleaching, purging worldview was to defy it: to wear scent and lipstick every day….". And here Nana pretty much fades from view. It's too bad, she was an interesting character. I suppose she was just to lend background to Mum, but it felt like she was abandoned by the storyteller.
Auntie Andy (aunt on disappeared father's side) comes to stay with Mum and Stella. This is stretched out a while, Stella in the dark about the reason, but after a day or two (and a page or so) we all find out: Uncle Derek, whose name Stella never knew because she never met him, killed their son Charlie. Stella never liked Charlie, he had "sly and hostile energy, full of contempt for girls and women." Which he probably learned from Uncle Derek who beat Auntie Andy regularly, and at the trial Stella notes that Derek's mother says something to give her the impression that his father beat his mother as well. So we have three generations of abusers, though Charlie never got his chance at bat, so to speak. It's a little advanced for an n 8-year-old to come up with this, but she is speaking from the vantage point of decades later.
I also found Stella's reaction to Charlie's death interesting. "I resented Charlie with a pure rage…. He seemed a usurper in a realm that gave him a huge advantage of pity and terror: he surely didn't belong there, with his ugly stamping feet." I had a similar reaction when I learned my ex-husband had died. How unfair! Now I was not allowed ever again to say anything mean about him!
Someone, I don't remember who or where, said recently of another story that it seemed a story of ideas rather than about the characters. That's what I think I get here. There are some great ideas here, about how women are treated, how they accept that treatment, and how (maybe) some things have changed a bit. The characters are well-drawn with great anecdotes and Stella's observations are wonderful. But… it doesn't feel like a great read to me. It feels like a sociology essay. I don't have a picture of Stella. Or of Mum or Andy or Nana. And it's very much a women-against-men world; I can't imagine a man reading this and not feeling ashamed. Oh, wait! No, feeling shame over someone else's behavior is what women do.
Tessa Hadley gives an interview in The New Yorker in which she says this is the first chapter of a novel-in-stories about Stella, which may account for the flatness of my experience. Excerpts tend to be background for the more interesting twists of future events in a novel. And I think that's it, this is great background, and I'm still waiting for the story to start.
Stella does not participate in her destiny. She can not, she is a child. It is not her destiny at stake! So she is not the central character! But she is the narrator and it feels like her story and it is confusing! Whose destiny is at stake? Auntie Andy of course, what do you do when your husband kills your child, you can lay down and die or you can have Honor and Dignity and find a new husband and get some kind of life back, since life was interrupted but it was not your fault! And that is what Auntie Andy does, except we see her through the eyes of a child remeniscing decades later so it is at a distance. But the story belongs to Andy, I think, and a little bit to Mum who participates in her destiny by letting Andy stay with them, giving Stella the view of two people, three if you count Nana. And she has these three role models of how to live. The problem is – and here is the problem – Stella does not show how these three role models affect her! We do not know! Because it is a novel in stories and we have not read that story yet! This is why novel excerpts do not work as short stories, I am afraid!
But of course that is just what I think. I hope other people will tell me what they think – hello? Is anyone out there?
This entry was posted in The New Yorker, What I've been Reading, Writing/Reading, Zin and tagged Tessa Hadley. Bookmark the permalink.


text:
'use strict';
/*@ngInject*/
/* global angular */
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  'ui.router',
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])
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I was searching for a Property and found this listing (MLS® #PW18261474). Please send me more information regarding 4625 E Cerro Vista Drive, Anaheim Hills, CA, 92807. Thank you!
I'd like to request a showing of 4625 E Cerro Vista Drive, Anaheim Hills, CA, 92807 (MLS® #PW18261474). Thank you!


text:
est un EP de David Bowie. Il se compose de six chansons rares ou inédites enregistrées entre 1995 et 1997, dont plusieurs chutes de l'album . Elles sont publiées en streaming par Parlophone du 8 janvier au 14 février 2020, à raison d'un titre par semaine.

Cet EP est également édité en vinyle et CD en édition limitée le 20 mars 2020. Sur ces supports physiques, la première version de  est remplacée par .

Histoire

 est publiée le 8 janvier. Elle fait partie des chansons enregistrées par Bowie pour l'émission de radio  diffusée par la BBC à l'occasion du cinquantième anniversaire du chanteur, le . Il s'agit de versions à dominante acoustique de plusieurs de ses chansons favorites.

 est publiée le 17 janvier. C'est une nouvelle version d'une composition de Bowie et Reeves Gabrels parue en 1989 sur le premier album du groupe Tin Machine. Le chanteur estime qu'il s'agit d'une de ses meilleures chansons et qu'elle mérite davantage de reconnaissance, ce qui l'incite à revenir dessus lors des séances d'enregistrement de . Cependant, il décide à la dernière minute de ne pas l'inclure sur l'album au profit de . Une autre version enregistrée au même moment est éditée en single et figure dans la bande originale du film .

 est publiée le 24 janvier. Cette chanson, hybride de rock, de soul et de funk, est apparue en 1976 sur l'album . Durant les répétitions préparatoires de la tournée , Bowie la fait jouer à son groupe dans un arrangement remis au goût du jour. Cette version répétée est enregistrée et peaufinée ultérieurement comme potentielle face B d'un single, mais elle n'est finalement pas utilisée.

 est publiée le 31 janvier. Cette composition de Bowie et Gabrels a paru à l'origine en ouverture du deuxième album de Tin Machine, en 1991, ainsi qu'en single. Le chanteur la reprend sur scène en solo lors du , en 1996, et décide d'en enregistrer une nouvelle version pour . Cette nouvelle version est censée figurer sur l'album entre  et , mais Bowie décide finalement de ne pas l'inclure.

 est publiée le 7 février. Issue de la dernière séance d'enregistrement de , en novembre 1996, elle est écartée de l'album à la dernière minute. Cette chanson quasi-instrumentale est la seule de l'EP qui ne soit pas une reprise d'un morceau déjà connu de Bowie.

 est publiée le 14 février. Il s'agit d'un enregistrement réalisé durant la tournée  et retravaillé en studio par Brian Eno. Sa première parution remonte à novembre 1995, en face A du single .

 trouve son origine dans la tournée . Au milieu de la chanson , la séquence  donne régulièrement lieu à une jam drum and bass. Retravaillée en studio, elle donne naissance à un nouveau titre, d'abord baptisé , puis simplement . Remixée par Danny Saber, elle est publiée de manière limitée en 1998. Un autre remix, le « Dillinja Mix », paraît en 1999 sur l'album .

Fiche technique

Titres

Streaming

Édition physique limitée

Musiciens

 David Bowie : chant
 Reeves Gabrels : guitares, synthétiseurs, chœurs
 Gail Ann Dorsey : basse et chœurs sur toutes les chansons sauf
 Mark Plati : claviers et programmation sur toutes les chansons sauf  et
 Mike Garson : piano et claviers sur , ,  et
 Zachary Alford : batterie sur , ,  et
 Carlos Alomar : guitare sur
 Peter Schwartz : synthétiseurs sur
 Brian Eno : chœurs sur

Classements

Références

Bibliographie

 .

Liens externes

EP de David Bowie
EP sorti en 2020

redpajama_set_name: RedPajamaWikipedia


text:
Q: Installing Oracle Database 11g Express Edition on Ubuntu I'm struggling to install Oracle 11g Express Edition on Ubuntu 14.04
I've followed every installations steps from the oracle manual, when i try to
run the /etc/init.d/oracle-xe configure, it gives me this error
root@server:/home/nuno# /etc/init.d/oracle-xe configure
Oracle Database 11g Express Edition Configuration
Specify the HTTP port that will be used for Oracle Application Express [8080]:8090
Specify a port that will be used for the database listener [1521]:1521
/etc/init.d/oracle-xe: line 405: /bin/awk: Is a directory
Specify a password to be used for database accounts.  Note that the same
password will be used for SYS and SYSTEM.  Oracle recommends the use of
different passwords for each database account.  This can be done after
initial configuration:
Confirm the password:
Do you want Oracle Database 11g Express Edition to be started on boot (y/n) [y]:y
Starting Oracle Net Listener...touch: cannot touch '/var/lock/subsys/listener': No such file or directory
Done
Configuring database...
Database Configuration failed.  Look into /u01/app/oracle/product/11.2.0/xe/config/log for details
This is the output of log file
CREATE OR REPLACE LIBRARY dbms_sumadv_lib AS '/u01/app/oracle/product/11.2.0/xe/lib/libqsmashr.so';
*
ERROR at line 1:
ORA-01034: ORACLE not available
Process ID: 0
Session ID: 0 Serial number: 0
BEGIN dbms_datapump_utl.replace_default_dir; END;
*
ERROR at line 1:
ORA-01034: ORACLE not available
Process ID: 0
Session ID: 0 Serial number: 0
commit
*
ERROR at line 1:
ORA-01034: ORACLE not available
Process ID: 0
Session ID: 0 Serial number: 0
create or replace directory XMLDIR as '/u01/app/oracle/product/11.2.0/xe/rdbms/xml'
*
ERROR at line 1:
ORA-01034: ORACLE not available
Process ID: 0
Session ID: 0 Serial number: 0
DROP DIRECTORY ORACLE_OCM_CONFIG_DIR
*
ERROR at line 1:
ORA-01034: ORACLE not available
Process ID: 0
Session ID: 0 Serial number: 0
DROP DIRECTORY ADMIN_DIR
*
ERROR at line 1:
ORA-01034: ORACLE not available
Process ID: 0
Session ID: 0 Serial number: 0
DROP DIRECTORY WORK_DIR
*
ERROR at line 1:
ORA-01034: ORACLE not available
Process ID: 0
Session ID: 0 Serial number: 0
BEGIN dbms_swrf_internal.cleanup_database(cleanup_local => FALSE); END;
*
ERROR at line 1:
ORA-01034: ORACLE not available
Process ID: 0
Session ID: 0 Serial number: 0
commit
*
ERROR at line 1:
ORA-01034: ORACLE not available
Process ID: 0
Session ID: 0 Serial number: 0

A: I struggled with this too for a while.  I followed the instructions on this pages:
detailed guide
another detailed guide.
A problem I ran into was that the sudo /etc/init.d/oracle-xe configure would fail towards the end.
I found, for me, that the net.ipv4.ip_local_port_range=9000 65000 in the /etc/sysctl.d/60-oracle.conf config file of the walk through was causing the configuration program to not configure the last step. I figured out the config file was causing it to not properly load an oracle instance, which than through the ORA-01034.  So, I just changed it to net.ipv4.ip_local_port_range=1 65000 left everything else the same and it worked no problem.
I think because the ports I was trying to use wasn't in the ip_local_port_range it was making it not connect.

redpajama_set_name: RedPajamaStackExchange


text:
Tag: Presidential Research Scholarship and Artistry Professorship
Faculty awards ceremony planned this afternoon
April 21, 2016 Mark McGowan Awards, Digital Signage, Events, Faculty & Staff, Latest News, On Campus
NIU President Doug Baker invites the entire university community to join him in congratulating the newly named Board of Trustees Professor, Presidential Research, Scholarship and Artistry Professors, Presidential Teaching Professor, Presidential Engagement Professor and the Excellence in Undergraduate Teaching and Instruction Award
Presidential Professorships enhanced, united call for nominations issued
September 8, 2015 Mark McGowan Awards, Faculty & Staff, Latest News
Faculty excellence in teaching, research, scholarship, artistry and engagement will be recognized in a bigger way beginning this year, as revisions to the Presidential Professorships are enacted. Base salary increments for the awards have been increased from $2,000 to $5,000, and colleges


text:
(895) Helio – planetoida należąca do zewnętrznej części pasa głównego asteroid okrążająca Słońce w ciągu 5 lat i 268 dni w średniej odległości 3,2 au. Została odkryta 11 lipca 1918 roku w Landessternwarte Heidelberg-Königstuhl w Heidelbergu przez Maxa Wolfa. Nazwa planetoidy pochodzi od pierwiastka helu, którego spektrum badali wspólnie Friedrich Paschen i Carl Runge (nazwę nadał Friedrich Paschen na prośbę odkrywcy). Przed nadaniem nazwy planetoida nosiła oznaczenie tymczasowe (895) 1918 DU.

Zobacz też
 lista planetoid 1–1000
 lista ponumerowanych planetoid

Bibliografia

Linki zewnętrzne

Planetoidy pasa głównego
Nazwane planetoidy
Obiekty astronomiczne odkryte w 1918


text:
Physical and Mathematical Modeling. Oil, Gas, Energy /
Adaptation of algorithm for calculating multicomponent system phase equilibrium for fields with uncertain initial data
Physical and Mathematical Modeling. Oil, Gas, Energy
№4 (20)
2020. Vol. 6
Bulletin of Tyumen State University. Physics and mathematics. Informatics (№4, 2012)
Tyumen State University Herald. Physical and Mathematical Modeling. Oil, Gas, Energy
Authors: Danila A. Kiselev, Alexander P. Shevelev, Alexander Ya. Gilmanov
For citation: Kiselev D. A., Shevelev A. P., Gilmanov A. Ya. 2019. "Adaptation of algorithm for calculating multicomponent system phase equilibrium for fields with uncertain initial data". Tyumen State University Herald. Physical and Mathematical Modeling. Oil, Gas, Energy, vol. 5, no 2, pp. 89-104. DOI: 10.21684/2411-7978-2019-5-2-89-104
Danila A. Kiselev, Postgraduate Student, Department of Modeling of Physical Processes and Systems, Institute of Physics and Technology, University of Tyumen; danilakis@rambler.ru
Alexander P. Shevelev, Cand. Sci. (Phys.-Math.), Professor, Department of Modeling of Physical Processes and Systems, Institute of Physics and Technology, University of Tyumen; eLibrary AuthorID, alexandershevelev@mail.ru
Alexander Ya. Gilmanov, Second Category Engineer, Department of Modeling of Physical Processes and Systems, Institute of Physics and Technology, University of Tyumen; a.y.gilmanov@utmn.ru
To date, hard-to-recover reserves are being actively developed; their majority are gas condensate fields. During the development of the field, the reservoir pressure drops, which leads to the retrograde condensation. Predicting these processes requires calculating phase behavior of hydrocarbons. The existing calculation algorithm requires long and expensive laboratory experiments to determine the properties of a group of heavy components. In many gas condensate fields, there was absence of studies of reservoir fluids at the initial stages of development. Additional laboratory studies are currently impossible due to the changes in the component composition during the development. Therefore, it is necessary to adapt the existing classical algorithm for fields with uncertainty of the initial data.
To solve this problem, it is necessary to determine a set of initial field data that characterizes the phase state of the reservoir fluid during development in a unique way. The authors have developed a consistent method of adapting the model of a multicomponent system to field data. The calculations used the Peng-Robinson cubic equation of state and the Lewis theory of a simplified description of phase equilibrium. Using the proposed algorithm, the content of gas condensate in the formation gas is calculated to predict the final condensate recovery factor. The dependence of the critical parameters of the group of heavy hydrocarbons on the main parameters of the phase transition is established and the necessary field data are identified. The algorithm was adopted for Zaykinsko-Zorinskoye field on the history of the development.
multicomponent system
gas condensate fields
PVT-model
equation of state
physical and mathematical modeling
phase equilibrium
critical parameters
retrograde condensation
Batalin O. Yu., Brusilovskiy A. I., Zakharov M. Yu. 1992. Phase Equilibria in Natural Hydrocarbons Systems]. Moscow: Nedra. [In Russian]
Brusilovskiy A. I. 2002. Phase Transformations in Oil and Gas Fields Development. Moscow: Graal. [In Russian]
Gimatudinov Sh. K., Shirkovskiy A. I. 1982. Physics of Oil and Gas Reservoir: Textbook. 3rd edition. Moscow: Nedra. [In Russian]
Korn G., Korn T. 1974. Mathematical Handbook for Scientists and Engineers. Translated from English; edited by I. G. Aramanovich. Moscow: Nauka. [In Russian]
Reid R., Prausnitz J., Sherwood T. 1982. Properties of Gases and Liquids. Translated from English; edited by B. I. Sokolov. 3rd edition, revised. Leningrad: Khimiya. [In Russian]
Sokolov V. S., Kiselev D. A., Smirnov A. Yu. 2016. "Method of forecasting of the coefficient of condensate recovery in fields with a low degree of scrutiny". Neftepromislovoe delo, no 4, pp. 5-9. [In Russian]
Sokolov V. S., Kiselev D. A., Smirnov A. Yu. 2017. "Simulation of phase equilibrium of gas-condensate systems for the fields with a low degree of scrutiny". Nedropolzovanie XXI vek, no 4, pp. 52-57. [In Russian]
Sokolov V. S., Kiselev D. A., Smirnov A. Yu. 2016. "Problems of providing condensate recovery factor of gas condensate objects on the example of porous-fractured reservoirs of Zaykinsko-Zorinskoye Field in the Orenburg Region". Neftepromislovoe delo, no 11, pp. 12-16. [In Russian]
Shirkovskiy A. I. 1987. Development and Operation of Gas and Gas Condensate Fields. Moscow: Nedra. [In Russian]
Thomas F. B., Bennion D. B., Andersen G. 2009. "Gas Condensate Reservoir Performance". Journal of Canadian Petroleum Technology, vol. 48, no 7, PETSOC-09-07-18. DOI: 10.2118/09-07-18


text:
import requests

from django.http import HttpResponse

def create_view(request):
    return HttpResponse(requests.get("http://captcha.seznam.cz/captcha.create").text)

def check_view(request, key, code):
    return HttpResponse(requests.get("http://captcha.seznam.cz/captcha.check?hash=%s&code=%s"%(key, code)).text)


The Russian Embassy in London says it will not respond until it receives samples of the chemical used in the attack on an ex-spy.
A deadline has passed for Vladimir Putin to explain Moscow's alleged use of a chemical weapon in Salisbury, with the UK and Russia seemingly at a stalemate.
Prime Minister Theresa May had given the Russian President until the end of Tuesday to confirm whether former spy Sergei Skripal and his daughter Yulia were poisoned in a state attack, or if Russia had "lost control" of the nerve agent used in the attempted murder.
The Russian Embassy in London, however, said it would not respond to Mrs May's deadline until it had received samples of the chemical used in the attack.
Possible retaliation from the UK could include sanctions, although the Russian Embassy in London claimed plans were "being developed to strike Russia with cyber weapons".
It warned that "any threat to take 'punitive' measures against Russia will meet with a response".
"The British side should be aware of that," it said.
"Britain must comply with the Chemical Weapons Convention which stipulates joint investigation into the incident, for which Moscow is ready."
Allies including the US, France, Germany, and countries bordering Russia - Latvia, Estonia and Lithuania - have lined up behind the UK to express their support.
As the deadline drew closer, the Foreign Office said: "[Boris Johnson] has emphasised that if this was a direct act by the Russian state then it would not simply be a threat to the UK, but a clear violation of the chemical weapons convention, a breach of international law and a threat to those who abide by the rules-based international order as a whole."
Mr Skripal, 66, is a former Russian spy who sold secrets to MI6 before being jailed in Russia.
He was released in a spy swap in 2010 and has lived in Britain since.
He lived an apparently quiet life until he and his 33-year-old daughter were found slumped on a bench in a shopping centre on 4 March - an attack Mrs May said was "highly likely" carried out by Russia.
Mr Skripal and his daughter remain in a critical condition in hospital.
A police officer who was among the first on the scene was also seriously affected but is recovering well.
In total, 38 people required treatment for the effects of nerve agent novichok.
Meanwhile, the UK's broadcasting regulator Ofcom has written to the Russian state-owned television channel RT as part of an investigation to assess if it is fit and proper to hold a broadcast licence.
In a statement, it said: "This letter explained that, should the UK investigating authorities determine that there was an unlawful use of force by the Russian State against the UK, we would consider this relevant to our ongoing duty to be satisfied that RT is fit and proper."


After the fiasco that was Iron Dog, most thought that young director Vincent Savio might consider a career change. Apparently not.
Savio had been keeping a low profile, until last week. He was seen in a rehearsal studio and was also rumored to have met with casting director Tim Trull. Finally, we confirmed yesterday that he will direct a new reading of his latest project.
Here's what we know – it's a new musical entitled Light Me Up. The show chronicles Thomas Edison and his efforts to control the motion picture industry during its early years. It's unclear as to whether Savio is writing the book and score himself or if he's working with a new team.
Theater Burn EXCLUSIVE: We've learned that Savio is not the first person to own this project. The original book/score was written by gentleman named Aaron Andrews, who has fallen into obscurity after being removed from the project. Andrews contacted us recently and gave us the behind the scenes story on the project's early stages.
According to Andrews, the producer who owned the rights to Light Me Up commissioned him to write the piece. All was going well, but tension between Andrews and the producer's wife at the time rose to epic proportions. Through a bizarre turn of events that we're still investigating, Andrews was ultimately fired from the project. Due to partial gag-order, Andrews was unable to give us any further details.
While working on the score, Andrews would routinely record scratch tracks of his songs for himself. He kept these recordings secret, figuring the project was dead, but with rumors of Savio's reading he decided to release them and tell the real story of the show's creation.
Savio's people have yet to comment on Andrew's version of the story, but that's not surprising. Since Iron Dog, the director has been avoiding interviews left and right. With this new reading, Savio has the chance to change the public perception of both him as a director and creator of new theater. We hope he understands the great opportunity he's been given and takes advantage of it.
I can't believe he has the nerve to do theater again!! He should publicly apologize to any person who saw – no, SUFFERED THROUGH – Iron Dog. What an a**!
Vincent is amazing. I don't have any sway with the critics, but I'm sure they're going to love this reading.
I still want my money back from Iron Dog!!
When is this reading going up?
I had the opportunity to audition for the Boston version of Iron Dog. It was such a rich piece and I wish I could have been a part of THAT production. What Savio did with it in New York was so far removed from the script that I question his ability to direct anything. I get the sense that regardless of the book, music, or lyrics, this show will be all about him.
Based on this recording, this guy should not sing rock. Ever.
I'm not sure he's actually a performer. It sounds like these were just demo tracks.
I'm totally looking forward to this show. Edison rules!! Hoping it's not an invite only reading.


residents interested in local history this month.
Archives and Museums (TWAM), are delivering special events, including talks and workshops, guided walking tours and exhibitions, celebrating Local History Month throughout May.
Tyne and Wear is a hotbed of curious tales and historical ghosts.
Blue Badge Guide and local history expert Jan Williams said; "For local history with national importance then residents need look no further than the fantastic heritage found throughout Tyne and Wear.
information on the Collingwood celebrations go to www.collingwood2010.co.uk.
A listing of events taking place across Tyne and Wear is attached.
love of Northumberland and the friends and family he left behind.
paid a record $36 million for Homer's landscape Lost On The Grand Banks and the painting Inside theBar, Cullercoats 1883 hangs in the Metropolitan Museum of Art, New York. In 1881, Homer paid a visit to Cullercoats, then a fishing village, and minor artist's colony. He stayed for almost two years. What brought him there, and why did he stay so long? Throughout May Locations across NewcastleGateshead www.visitnewcastlegateshead.co.uk NewcastleGateshead's guided tours are free throughout local history month, themes include Newcastle's Hidden Art, Seedy and Sophisticated and In Sickness And In Health.


text:
The Sacred Heart Way
A School For Girls
Mercy Education Limited
Learning @ SHC
Our Learning Philosophy
IB Middle Years Program
PA40+
The Bradbury Club
Entrepreneurship: Pitch Perfect
myLearning Journey
Coronavirus Information Updates
SHC In The Media
Enrolments Overview
Family Life @ SHC
Enrolment Applications
Online Discovery Day
Gift of a Rose
Class Gifts
Also in this section /
In 2003 the College implemented the International Baccalaureate Middle Years Program, and in 2004 Sacred Heart was authorised as an IB World School.
The Middle Years Program is based on, and reflects, current research conducted on Middle Years schooling.
This program is designed to assist students to become independent learners who can recognise relationships between school subjects and the world outside, who can adapt to new situations and combine relevant knowledge, practical and social intelligence to solve authentic problems individually or in groups.
The Program aims to enable students to:
build upon their spirit of discovery to develop an understanding and enjoyment of learning, independently and in cooperation with others.
acquire knowledge and understanding and prepare for further learning.
recognise the extent to which knowledge is interrelated.
learn to communicate effectively in a variety of ways.
develop a sense of personal and cultural identity and a respect for themselves and for others.
acquire insights into local and global concerns affecting health, the community and the environment, and develop a sense of individual and collective responsibility and citizenship.
The central concepts of the Program are:-
Holistic Learning
Intercultural Awareness
The aim of all IB programs is to develop internationally minded people who, recognising their common humanity and shared guardianship of the planet, help to create a better and more peaceful world.
IB learners strive to be:
These aspects of the program make it consistent with the College's aims. At Sacred Heart College students complete studies in nine subject groups.
Language A (English)
Languages (a Language Other Than English)
Humanities (History, Geography, Commerce)
The Arts (Visual and Performing Arts)
Design, Creativity and Technology (Design Technology and Information, Communication Technology)
Health and Physical Education.
In the final year of the IB MYP students complete a Personal Project. It is an individual and formal expression of what the student has learned during their years in the MYP. It is based in one of the Global Contexts and reflects a topic of real interest to the individual student. It is completed outside normal timetabled classes and is supervised by a member of the SHC teaching staff.
For more information, please visit the IB website by clicking here: IB Middle Years Program
Family Life@SHC
https://sacredheartcollege.instructure.com/courses/2295/
/enrolment/enrolment-application-process.html
/LearningatSHC/our-learning-philosophy
Retreat Road, NEWTOWN 3220 Victoria
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CHARLESTON, S.C. - South Carolina's Department of Juvenile Justice took a 13-year-old boy into custody after another student handed a teacher a note saying the teen...
RENO, Nev. (AP) — A pigeon wearing a...
State puts out call for more foster parents
4 years 2 months 3 weeks ago Tuesday, October 27 2015 Oct 27, 2015 October 27, 2015 5:05 PM October 27, 2015 in News
By: Russell Jones, Ambria Washington
BATON ROUGE - State officials are asking more people to consider becoming foster parents to help find homes for a growing number of children in Louisiana's foster care system.
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Secretary Suzy Sonnier with the Department of Children and Family Services said there are close to 5,000 children in the program today, a 13 percent increase from three years ago.
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Currently, Louisiana serves 4600 children a month in foster care. Foster parents must meet a number of qualifications, including being 21 or older and having a sufficient income.
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South Ardenwood, Baton Rouge on Thursday November 5th at 6:00 p.m. There are a number of other orientations coming up in November and December across the state. You can find a list of
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\begin{document}

\markboth{Eduardo Guendelman, Emil Nissimov, Svetlana Pacheva}
{Gravity-Assisted Emergent Higgs Mechanism in the Post-Inflationary Epoch}

\catchline{}{}{}{}{}

\title{\textbf{GRAVITY-ASSISTED EMERGENT HIGGS MECHANISM IN THE
POST-INFLATIONARY EPOCH}
\foot{Honorable Mention in the Gravity Research Foundation Essay Competition 2016}
}

\author{Eduardo Guendelman}

\address{Department of Physics, Ben-Gurion University of the Negev,
Beer-Sheba 84105, Israel \\
guendel@bgu.ac.il}

\author{Emil Nissimov, Svetlana Pacheva}
\address{Institute for Nuclear Research and Nuclear Energy,\\
Bulgarian Academy of Sciences, Sofia 1784, Bulgaria\\
nissimov@inrne.bas.bg , svetlana@inrne.bas.bg}

\date{March 20, 2016}
\maketitle

\maketitle

\begin{history}
\received{}
\revised{}
\end{history}

\begin{abstract}
We consider a non-standard model of gravity coupled to a neutral scalar
``inflaton'' as well as to $SU(2)\times U(1)$ iso-doublet scalar with positive mass
squared and without self-interaction, and to  $SU(2)\times U(1)$ gauge fields.
The principal new ingredient is employing two alternative non-Riemannian
space-time volume-forms (covariant
integration measure densitities) independent of the metric. The latter have
a remarkable impact -- although not introducing any additional propagating
degrees of freedom, their dynamics triggers a series of important features:
appearance of infinitely large flat regions of the effective ``inflaton''
potential as well as dynamical generation of Higgs-like spontaneous symmetry breaking
effective potential for the $SU(2)\times U(1)$ iso-doublet scalar.
\end{abstract}

\keywords{non-Riemannian volume forms; quintessential evolution; dynamical generation of electroweak
symmetry breaking.}

\ccode{PACS numbers:04.50.Kd,
11.30.Qc,
}

\section{Introduction}
\label{intro}

In a remarkable paper from 1986 \ct{bekenstein} J. Bekenstein proposed the
intriguing idea about a gravity-assisted spontaneous symmetry breaking of
electro-weak (Higgs) type without invoking unnatural (according to
Bekenstein's opinion) ingredients like negative mass squared and a quartic
self-interaction for the Higgs field. By considering a model of gravity interacting
with a standard Klein-Gordon field (with small positive mass squared and
without self-interaction) coupled conformally to the scalar
curvature he managed to obtain a prototype of dynamically induced Higgs-like
spontaneous symmetry breaking scalar potential. A similar approach was further
worked out in Ref.~\refcite{moniz-etal}.

Motivated by Bekenstein's idea, in the present essay we will consider a
non-standard model of gravity coupled to a neutral scalar ``inflaton'' $\vp$ as
well as to a $U(1)$-charged $SU(2)$ iso-doublet scalar field $\s$ with a
standard positive mass squared and no self-interaction, as well as to
$SU(2)\times U(1)$ gauge fields. The essential non-standard feature of this
model is employing non-Riemannian space-time volume forms -- alternative generally
covariant integration measure densities defined in terms of auxiliary
antisymmetric tensor gauge fields independent of the pertinent Riemannian
metric\foot{The method of non-Riemannian space-time volume forms,
originally proposed in Refs.~\refcite{TMT-orig-1,TMT-orig-2} has been employed in a broad
variety of gravity-matter, supergravity and strings/branes models to provide
plausible solutions for dynamical generation of cosmological constant, the
supersymmetric Higgs effect \ct{susyssb}, unified description of early
universe inflation and present day dark energy \ct{emergent}, unified description
of dark energy and dark matter as different manifestations of a single entity
\ct{dusty-1,dusty-2}}.
Although being almost pure-gauge degrees of freedom (see the remark
in Section 2 below), the non-Riemannian space-time volume forms trigger a
series of important features unavailable in ordinary gravity-matter models
with the standard Riemannian volume-form (given by the square-root of the determinant
of the Riemannian metric): (i) The ``inflaton'' $\vp$ develops a remarkable
effective scalar potential in the Einstein frame possessing an infinitely
large flat region for large negative $\vp$ describing the ``early'' universe
evolution; (ii) In the absence of the $SU(2)\times U(1)$ iso-doublet scalar field, the
``inflaton'' effective potential has another infinitely large flat region for
large positive $\vp$ describing the ``late'' post-inflationary
(dark energy dominated) universe;
(iii) Inclusion of the $SU(2)\times U(1)$ iso-doublet scalar field $\s$ introduces a
drastic change in the total effective scalar potential in the post-inflationary
universe -- the effective potential as a function of $\s$ acquires exactly
the electro-weak Higgs-type spontaneous symmetry breaking form.

\section{Gravity-Gauge-Field-Matter Model With Two Independent Non-Riemannian
Volume-Forms}
\label{TMMT}
Our starting point is the following non-standard gravity-gauge-field-matter system
with an action of the general form involving two independent non-Riemannian
volume-forms
generalizing the model studied in Ref.~\refcite{emergent} and whose gauge-field-matter
part has an internal $SU(2)\times U(1)$ gauge symmetry (for simplicity
we will use units where the Newton constant is taken as $G_{\rm Newton} = 1/16\pi$):
\be
S = \int d^4 x\,\P_1 (A) \Bigl\lb R - 2\L_0 \frac{\P_1 (A)}{\sqrt{-g}}
+ L^{(1)} \Bigr\rb + \int d^4 x\,\P_2 (B) \Bigl\lb L^{(2)} +
\frac{\P (H)}{\sqrt{-g}}\Bigr\rb \; .
\lab{TMMT}
\ee
In \rf{TMMT} and in the sequel the following notations are used:

\begin{itemize}
\item
$\P_{1}(A)$ and $\P_2 (B)$ are two independent non-Riemannian volume-forms,
\textsl{i.e.}, alternative generally covariant integration measure densities on
the underlying space-time manifold:
\be
\P_1 (A) = \frac{1}{3!}\vareps^{\m\n\k\l} \pa_\m A_{\n\k\l} \quad ,\quad
\P_2 (B) = \frac{1}{3!}\vareps^{\m\n\k\l} \pa_\m B_{\n\k\l} \; ,
\lab{Phi-1-2}
\ee
defined in terms of field-strengths of two auxiliary 3-index antisymmetric
tensor gauge fields. $\P_{1,2}$ take over the role of the standard Riemannian
integration measure density
$\sqrt{-g} \equiv \sqrt{-\det\Vert g_{\m\n}\Vert}$ in terms of the space-time
metric $g_{\m\n}$.
\item
$R = g^{\m\n} R_{\m\n}(\G)$ and $R_{\m\n}(\G)$ are the scalar curvature and the
Ricci tensor in the first-order (Palatini) formalism, where the affine
connection $\G^\m_{\n\l}$ is \textsl{a priori} independent of the metric $g_{\m\n}$.
$\L_0$ is a small
parameter later to be
identified with the present epoch small observable cosmological constant.
\item
$L^{(1)}$ is the sum of two scalar field Lagrangians:
\be
L^{(1)} = -\h g^{\m\n} \pa_\m \vp \pa_\n \vp - V_1(\vp) -
g^{\m\n} \bigl(\nabla_\m \s_a)^{*}\nabla_\n \s_a - V_0 (\s) \; ,
\lab{L-1}
\ee
where $\vp$ denotes the neutral ``inflaton'' inert under $SU(2)\times U(1)$
and $\s \equiv (\s_a)$
is a complex $SU(2)\times U(1)$ iso-doublet scalar field
with the isospinor index $a=+,0$ indicating the corresponding $U(1)$ charge.
The gauge-covariant derivative in \rf{L-1} acting on the iso-doublet scalar $\s$ reads:
\be
\nabla_\m \s =
\Bigl(\pa_\m - \frac{i}{2} \t_A \cA_\m^A - \frac{i}{2} \cB_\m \Bigr)\s \; ,
\lab{cov-der}
\ee
with $\h \t_A$ ($\t_A$ -- Pauli matrices, $A=1,2,3$) indicating the $SU(2)$
generators and $\cA_\m^A$ ($A=1,2,3$)
and $\cB_\m$ denoting the corresponding $SU(2)$ and $U(1)$ gauge fields.
The pertinent scalar field potentials are:
\be
V_1 (\vp) = f_1 \exp \{-\a\vp\} \quad ,\quad
V_0 (\s) = m^2_0\, \s^{*}_a \s_a \; ,
\lab{V-1-0}
\ee
where $\a, f_1$ are dimensionful positive parameters, and $V_0 (\s)$ is just the
standard mass term for the iso-doublet $\s_a$ with positive mass squared.
\item
$L^{(2)}$ is the sum of a second ``inflaton'' Lagrangian plus the canonical
Lagrangians for the $SU(2)$ and $U(1)$ gauge fields $\cA^A_\m$, $\cB_\m$:
\be
L^{(2)} = -\frac{b}{2} e^{-\a\vp} g^{\m\n} \pa_\m \vp \pa_\n \vp + U(\vp)
- \frac{1}{4g^2} F^2(\cA) - \frac{1}{4g^{\pr\,2}} F^2(\cB) \; ,
\lab{L-2}
\ee
where:
\be
U(\vp) = f_2 \exp \{-2\a\vp\} \; ,
\lab{U}
\ee
with $f_2$ another dimensionful positive parameter, whereas $b$ is a
dimensionless one, and (all indices $A,B,C = (1,2,3)$):
\br
F^2(\cA) \equiv F^A_{\m\n} (\cA) F^A_{\k\l} (\cA) g^{\m\k} g^{\n\l} \quad ,\quad
F^2(\cB) \equiv F_{\m\n} (\cB) F_{\k\l} (\cB) g^{\m\k} g^{\n\l} \; ,
\lab{F2-def} \\
F^A_{\m\n} (\cA) =
\pa_\m \cA^A_\n - \pa_\n \cA^A_\m + \eps^{ABC} \cA^B_\m \cA^C_\n \quad ,\quad
F_{\m\n} (\cB) = \pa_\m \cB_\n - \pa_\n \cB_\m \; .
\lab{F-def}
\er
\item
$\P (H)$ indicates the dual field strength of a third auxiliary 3-index antisymmetric
tensor gauge field:
\be
\P (H) = \frac{1}{3!}\vareps^{\m\n\k\l} \pa_\m H_{\n\k\l} \; ,
\lab{Phi-H}
\ee
whose presence is crucial for non-triviality of the model.
\end{itemize}

\textbf{Remark.} The systematic canonical Hamiltonian treatment of \rf{TMMT}
(see {\em Appendix}) and, more
generally, of any gravity-matter models built with non-Riemannian volume-forms
\ct{buggy} shows that the auxiliary 3-index tensor gauge fields $A_{\m\n\k}$,
$B_{\m\n\k}$, $H_{\m\n\k}$ are almost pure-gauge, \textsl{i.e.}, they do not
introduce any new propagating field degrees of freedom except for a few
free integration constants in their respective equations of motion (see
\rf{A-B-H-eqs}-\rf{integr-const} below).

Let us note that the requirement for invariance (with the exception of the mass
term $V_0 (\s)$ of the iso-doublet $\s_a$) under the following global Weyl-scale
symmetry:
\br
g_{\m\n} \to \l g_{\m\n} \;\; ,\;\; \vp \to \vp + \frac{1}{\a}\ln \l \;\;,\;\;
A_{\m\n\k} \to \l A_{\m\n\k} \;\; ,\;\; B_{\m\n\k} \to \l^2 B_{\m\n\k} \; ,
\lab{scale-transf} \\
\G^\m_{\n\l} \;,\; H_{\m\n\k} \;,\; \s_a \; ,\; \cA^A_\m \; ,\; \cB_\m \;
- \; {\rm inert} \; , \phantom{aaaaaaaaaaaa}
\nonu
\er
uniquely fixes the structure of the non-Riemannian-measure gravity-gauge-field-matter
action \rf{TMMT}. In particular, for the same reason we have multiplied by an
appropriate exponential factor the ``inflaton'' kinetic term in $L^{(2)}$ \rf{L-2}.

Following Ref.~\refcite{emergent} we will now derive the effective Einstein-frame form
of the dynamics described by \rf{TMMT}.

Variation of the action \rf{TMMT} w.r.t. affine connection $\G^\m_{\n\l}$:
\be
\int d^4\,x\,\sqrt{-g} g^{\m\n} \Bigl(\frac{\P_1}{\sqrt{-g}}\Bigr)
\(\nabla_\k \d\G^\k_{\m\n} - \nabla_\m \d\G^\k_{\k\n}\) = 0
\lab{var-G}
\ee
shows
that $\G^\m_{\n\l}$ becomes a Levi-Civita connection
$ \G^\m_{\n\l} = \G^\m_{\n\l}({\bar g}) =
\h {\bar g}^{\m\k}\(\pa_\n {\bar g}_{\l\k} + \pa_\l {\bar g}_{\n\k}
- \pa_\k {\bar g}_{\n\l}\)$
w.r.t. to the Weyl-rescaled metric ${\bar g}_{\m\n}$:
\be
{\bar g}_{\m\n} = \chi_1 \, g_{\m\n} \quad ,\quad
\chi_1 \equiv \frac{\P_1 (A)}{\sqrt{-g}} \; .
\lab{bar-g}
\ee

Variation of \rf{TMMT} w.r.t. auxiliary tensor gauge fields
$A_{\m\n\l}$, $B_{\m\n\l}$ and $H_{\m\n\l}$ yields the equations (using the
short-hand notation $\chi_1$ from \rf{bar-g}):
\be
\pa_\m \Bigl\lb R + L^{(1)} - 4\L_0 \chi_1\Bigr\rb = 0 \quad, \quad
\pa_\m \Bigl\lb L^{(2)} + \frac{\P (H)}{\sqrt{-g}}\Bigr\rb = 0
\quad, \quad \pa_\m \Bigl(\frac{\P_2 (B)}{\sqrt{-g}}\Bigr) = 0 \; ,
\lab{A-B-H-eqs}
\ee
whose solutions read:
\br
\frac{\P_2 (B)}{\sqrt{-g}} \equiv \chi_2 = {\rm const} \;\; ,\;\;
R + L^{(1)} - 4\L_0 \chi_1\ = - M_1 = {\rm const} \; ,
\nonu \\
L^{(2)} + \frac{\P (H)}{\sqrt{-g}} = - M_2  = {\rm const} \; .
\lab{integr-const}
\er
Here $M_1$ and $M_2$ are arbitrary dimensionful and $\chi_2$
arbitrary dimensionless integration constants.

Now, varying \rf{TMMT} w.r.t. $g_{\m\n}$ and using relations \rf{integr-const}
we obtain:
\be
\chi_1 \Bigl\lb R_{\m\n} + \h\( g_{\m\n}L^{(1)} - T^{(1)}_{\m\n}\) -
\L_0 \chi_1 g_{\m\n}\Bigr\rb -
\h \chi_2 \Bigl\lb T^{(2)}_{\m\n} + g_{\m\n} M_2 \Bigr\rb = 0 \; ,
\lab{pre-einstein-eqs}
\ee
where $\chi_1$ and $\chi_2$ are the same as in \rf{bar-g} and \rf{integr-const},
respectively, and $T^{(1,2)}_{\m\n}$ are the energy-momentum tensors of the
matter-gauge-field Lagrangians \rf{L-1}-\rf{L-2} with the standard definitions:
$T^{(1,2)}_{\m\n} = g_{\m\n} L^{(1,2)} - 2 \pa L^{(1,2)}/\pa g^{\m\n}$.

Taking the trace of Eqs.\rf{pre-einstein-eqs} and using again the second relation
\rf{integr-const} we solve for the scale factor $\chi_1$ \rf{bar-g}:
\be
\chi_1 = 2 \chi_2 \frac{T^{(2)}/4 + M_2}{L^{(1)} - T^{(1)}/2 - M_1}
\quad ,\quad T^{(1,2)} = g^{\m\n} T^{(1,2)}_{\m\n} \; .
\lab{chi-1}
\ee

Using the second relation \rf{integr-const}, the gravity equations \rf{pre-einstein-eqs}
can be put in the Einstein-like form:
\be
R_{\m\n} - \h g_{\m\n}R = \h g_{\m\n}\(L^{(1)} + M_1 - 2 \L_0 \chi_1\)
+ \h\(T^{(1)}_{\m\n} - g_{\m\n}L^{(1)}\)
+ \frac{\chi_2}{2\chi_1} \Bigl\lb T^{(2)}_{\m\n} + g_{\m\n} M_2 \Bigr\rb \; ,
\lab{einstein-like-eqs}
\ee

Now, using expression \rf{chi-1} for $\chi_1$ and following
the same steps as in Ref.~\refcite{emergent} we can bring Eqs.\rf{einstein-like-eqs}
into the standard form of Einstein
equations for the rescaled  metric ${\bar g}_{\m\n}$ \rf{bar-g},
\textsl{i.e.}, the Einstein-frame gravity equations:
\be
R_{\m\n}({\bar g}) - \h {\bar g}_{\m\n} R({\bar g}) = \h T^{\rm eff}_{\m\n}
\quad ,\quad
T^{\rm eff}_{\m\n} = g_{\m\n} L_{\rm eff} - 2 \partder{}{g^{\m\n}} L_{\rm eff}
\; ,
\lab{eff-einstein-eqs}
\ee
with effective energy-momentum tensor corresponding
to the following effective Einstein-frame matter Lagrangian:

\be
L_{\rm eff} = A(\vp,\s) X + B(\vp) X^2 - U_{\rm eff}(\vp,\s)
- {\bar g}^{\m\n} \bigl(\nabla_\m \s_a)^{*}\nabla_\n \s_a
- \frac{\chi_2}{4g^2} {\bar F}^2(\cA) - \frac{\chi_2}{4g^{\pr\,2}} {\bar F}^2(\cB)
\; .
\lab{L-eff-final}
\ee

In \rf{L-eff-final} the following notations are used:

\begin{itemize}
\item
$X$ is the standard short-hand notations for the ``inflaton'' kinetic term:
\be
X \equiv - \h {\bar g}^{\m\n}\pa_\m \vp \pa_\n \vp \; .
\lab{X-def}
\ee
\item
The coefficient functions in the ``k-essence''-type
\ct{k-essence-1,k-essence-2,k-essence-3,k-essence-4} expression
(first two terms on the r.h.s. of \rf{L-eff-final} with {\em non-linear} functional
dependence on $X$ \rf{X-def})
are given by:
\br
A(\vp,\s) \equiv 1 + \h b e^{-\a\vp}\,
\frac{V_1 (\vp) + V_0 (\s) - M_1}{U(\vp) + M_2}
\nonu\\
= 1 + \h b e^{-\a\vp}\,
\frac{f_1 e^{-\a\vp} + m_0^2 \s_a^{*}\s_a - M_1}{f_2 e^{-2\a\vp} + M_2} \; ;
\lab{A-def}
\er
and
\be
B(\vp) \equiv - \frac{1}{4}\,\frac{\chi_2 b^2 e^{-2\a\vp}}{U(\vp) + M_2}
= - \frac{1}{4}\,\frac{\chi_2 b^2 e^{-2\a\vp}}{f_2 e^{-2\a\vp} + M_2} \; .
\lab{B-def}
\ee
\item
The full effective scalar field potential reads:
\br
U_{\rm eff} (\vp,\s) \equiv
\frac{\Bigl\lb V_1(\vp) + V_0 (\s) - M_1 \Bigr\rb^2}{
4\chi_2 \Bigl\lb U(\vp) + M_2\Bigr\rb} + 2\L_0
\nonu\\
= \frac{\(f_1 e^{-\a\vp} + m_0^2 \s_a^{*}\s_a - M_1\)^2}{4\chi_2\,\Bigl\lb
f_2 e^{-2\a\vp} + M_2\Bigr\rb} + 2\L_0\; ,
\lab{U-eff}
\er
where in\rf{A-def}-\rf{U-eff} the explicit forms of $V_1 (\vp), V_0 (\s)$ and
$U(\vp)$ \rf{L-1}-\rf{L-2} are inserted.
\item
In the last line of \rf{L-eff-final} the Einstein-frame versions of the
gauge-field Lagrangians are used, where:
\be
{\bar F}^2(\cA) \equiv F^A_{\m\n} (\cA) F^A_{\k\l} (\cA) {\bar g}^{\m\k} {\bar g}^{\n\l}
\quad ,\quad
{\bar F}^2(\cB) \equiv F_{\m\n} (\cB) F_{\k\l} (\cB) {\bar g}^{\m\k} {\bar g}^{\n\l} \; .
\lab{bar-F2-def}
\ee
\end{itemize}

\section{Effective Scalar Potential -- Infinitely Large Flat Regions and
Emergent Higgs-like Behavoir}
\label{flat+higgs}

A remarkable feature of the effective Einstein-frame scalar potential \rf{U-eff}
is that it possesses an infinitely large flat region for large negative
$\vp$ and is independent of $\s$ there:
\br
U_{\rm eff}(\vp,\s) \simeq U_{(-)} \equiv \frac{f_1^2}{4\chi_2\, f_2} + 2\L_0
\; , \phantom{aaaaaaaaaaaa}
\lab{minus-region} \\
A(\vp,\s) \simeq A_{(-)} \equiv 1+\h b \frac{f_1}{f_2} \;\; ,\;\;
B(\vp) \simeq B_{(-)} \equiv - \chi_2 \frac{b^2}{4f_2} \; .
\nonu
\er
Thus, for large negative values of the ``inflaton'' the effective matter
Lagrangian \rf{L-eff-final} reads:
\br
L_{\rm eff}^{(-)} = A_{(-)} X + B_{(-)} X^2 - U_{(-)} + L\lb\s,\cA,\cB\rb \; ,
\lab{L-minus} \\
L\lb\s,\cA,\cB\rb \equiv
- {\bar g}^{\m\n} \bigl(\nabla_\m \s_a)^{*}\nabla_\n \s_a
- \frac{\chi_2}{4g^2} {\bar F}^2(\cA) - \frac{\chi_2}{4g^{\pr\,2}} {\bar F}^2(\cB) \; ,
\lab{L-sigma-gauge-def}
\er
\textsl{i.e.}, the $SU(2)\times U(1)$ iso-doublet scalar $\s$ becomes massless.

For large positive values of $\vp$ we obtain
$A(\vp,\s) \simeq A_{(+)} = 1$ , $ B(\vp) \simeq B_{(+)} = 0$, and:
\be
U_{\rm eff}(\vp,\s) \simeq U_{(+)}(\s) \equiv
\frac{1}{4\chi_2\, M_2} \Bigl( m_0^2 \s_a^{*} \s_a - M_1\Bigr)^2 + 2\L_0 \; ,
\lab{plus-region}
\ee
so that the effective matter Lagrangian \rf{L-eff-final} becomes
(using notation \rf{L-sigma-gauge-def}):
\be
L_{\rm eff}^{(+)} = X  - U_{(+)}(\s) + L\lb\s,\cA,\cB\rb \; .
\lab{L-plus}
\ee

In the case of absent $SU(2)\times U(1)$ scalar and gauge fields, a case
already discussed in detail in Ref.~\refcite{emergent}, the purely ``inflaton'' effective
potential $U_{\rm eff}(\vp) = \( f_1 e^{-\a\vp} - M_1\)^2
\llb 4\chi_2\,\bigl( f_2 e^{-2\a\vp} + M_2\bigr)\rrb^{-1}$
possesses another infinitely large flat region for large positive values of $\vp$:
$U_{\rm eff}(\vp) \simeq U_{(+)} \equiv M_1^2\, \(4\chi_2\, M_2\)^{-1}$
and the shape of $U_{\rm eff}(\vp)$
is depicted in Fig.1.

\begin{figure}
\begin{center}
\includegraphics{Effective-potential_2.eps}
\caption{Qualitative shape of the effective ``inflaton'' potential $U_{\rm eff}(\vp)$
as function of $\vp$, $M_1 > 0$.}
\end{center}
\end{figure}

It was found in Ref.~\refcite{emergent} that this effective ``inflaton'' potential
with two infinitely large flat regions with vastly different scales upon
appropriate choice for the values of the parameters accomodates the
description simultaneously of the ``early'' universe evolution (the inflationary
epoch) corresponding to the first flat region for large negative
$\vp$-values (the left one on Fig.1), as well as the ``late'' post-inflationary
(dark energy dominated) universe corresponding to the second flat region for large
positive $\vp$-values (the right one on Fig.1).

The presence of the $SU(2)\times U(1)$ scalar and gauge fields will not affect
significantly the inflationary dynamics in the ``early'' universe (when $\vp$ runs
on the left higher flat region of $U_{\rm eff}(\vp)$, Fig.1), and where
the $SU(2)\times U(1)$ iso-doublet $\s$-field is massless, see
\rf{L-sigma-gauge-def})) --
this dynamics is governed by the purely kinetic ``k-essence'' ``inflaton'' part
$A_{(-)} X + B_{(-)} X^2 - U_{(-)}$ of \rf{L-minus}.

However, in the post-inflationary epoch (when $\vp$ runs on the right lower flat
region of $U_{\rm eff} (\vp)$, Fig.1) the presence of the $SU(2)\times U(1)$
iso-doublet $\s$ contributes very significantly to the full effective scalar potential
\rf{plus-region}, which emerges in an exactly Higgs-like form:
\br
U_{(+)}(\s) =
\frac{1}{4\chi_2\, M_2} \Bigl( m_0^2 \s_a^{*} \s_a - M_1\Bigr)^2 + 2\L_0
\equiv
\l\, \bigl(\s_a^{*}\s_a\bigr)^2 - \m^2 \s_a^{*}\s_a + {\rm const} \; ,
\lab{higgs-like} \\
\l = \frac{m_0^4}{4\chi_2\,M_2} \quad ,\quad
\m^2 = \frac{M_1\,m_0^2}{2\chi_2\,M_2} \; . \phantom{aaaaaaaaaaaaaaaa}
\lab{higgs-param}
\er
Spontaneous $SU(2)\times U(1)$ symmetry breakdown occurs at the vacuum value:
\be
|\s_{\rm vac}| = \frac{1}{m_0}\sqrt{M_1} \; ,
\lab{s-vac}
\ee
with a small residual cosmological constant $\L_0$, which is identified with the
current epoch observable cosmological constant. Let us also note that
in the post-inflationary epoch according to \rf{L-plus} and \rf{higgs-like}
the massless ``inflaton'' $\vp$ (entering the kinetic term $X$ \rf{X-def} only)
looses all interactions with the $SU(2)\times U(1)$ iso-doublet $\s$
(which has now become the Higgs field), thus avoiding undesirable fifth-force problems.

The dependence of the Higgs-like parameters \rf{higgs-param} and the Higgs-like
v.e.v. \rf{s-vac} on the integration constants $M_{1,2}$ and $\chi_2$ explicitly
reveals the nature of the Higgs-like spontaneous gauge symmetry breaking
\rf{higgs-like} as a
gravity-assisted
dynamically generated phenomenon in the post-inflationary epoch.
It is triggered exclusively through the special non-Riemannian volume-form dynamics
in the original gravity-gauge-field-matter action \rf{TMMT} leading to the
remarkable two-flat-region shape of the ``inflaton'' effective potential (Fig.1).
Let us stress again that in the ``early'' universe there is no spontaneous
breaking of $SU(2)\times U(1)$ gauge symmetry and the Higgs-like iso-doublet
scalar field $\s$ is massless there \rf{L-minus}-\rf{L-sigma-gauge-def}.

We conclude with a note on the plausible numerical values for some of the
parameters involved. In Ref.~\refcite{emergent} it was argued that it is natural
to associate $M_1 \sim M^4_{EW}$, $M_2 \sim M^4_{Pl}$ and $\chi_2 \sim 10^{-1}$,
where $M_{EW}$ and $M_{Pl}$ are the electroweak and Planck scales, respectively.
Then, from \rf{s-vac} we see that it is natural also to associate the bare
mass of the $SU(2)\times U(1)$ iso-doublet $\s$-field $m_0 \sim M_{EW}$, so
that we will have for the Higgs-like v.e.v. $|\s_{\rm vac}| \sim M_{EW}$
conforming to the standard electroweak phenomenology.

\section*{Acknowledgements}
We gratefully acknowledge support of our collaboration through the academic exchange
agreement between the Ben-Gurion University and the Bulgarian Academy of Sciences.
S.P. and E.N. have received partial support from European COST actions
MP-1210 and MP-1405, respectively, as well from Bulgarian National Science
Fund Grant DFNI-T02/6. We also thank the referee for useful remarks and typo
corrections.

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