text:
Search results for "Jason Isbell"
Jason Isbell
Jason Isbell brings 400 Unit to Nashville (2017)
October 13, 2017 - Jason Isbell and the 400 Unit will be on stage at the Ryman in Nashville, TN
On web TV today, Jason Isbell and Amanda Shires at 'Tiny Desk (Home) Concert' (2020)
September 30, 2020 - if in front of a computer, do not miss Jason Isbell (voc, g) and his wife Amanda Shires (voc,…
On TV today, Jason Isbell with Charlie Rose (2017)
July 3, 2017 - you do not want to miss country singer Jason Isbell promoting his sixth album "The Nashville Sound"…
On Web TV today, Jason Isbell & Amanda Shires are live from Nashville (2020)
May 15, 2020 - if in front of a computer, do not miss Jason Isbell and Amanda Shires performing live for Relix…
Jason Isbell takes the 400 Unit to Orlando (2018)
April 18, 2018 - Jason Isbell and the 400 Unit will be on stage (and on Live Streaming) at The Walt Disney Theater…
Kacey, Jason, John et al are at Grand Ole Opry (2016)
December 31, 2016 - Kacey Musgraves, John Prine, Amanda Shires, Jason Isbell and more. They all will spend New…
Amanda Shires performs in Nashville (2019)
October 18, 2019 - American singer and fiddle player Amanda Shires opens for Jason Isbell at the Ryman in…
Roger Waters, Fleet Foxes, Yard Act, Idles, Brittany Howard, Goat Girl, Foo Fighters, Julia Michaels, Valerie June,…
Foo Fighters, Pale Waves, OneRepublic, Donovan Woods, Lindsey Stirling, Måneskin, NEEDTOBREATHE, Amanda Shires, Goo…
Tommy Emmanuel' s 'Accomplice One'
Tommy Emmanuel' s 'Accomplice One' is his twenty sixth studio album featuring guests such as Jason Isbell, Mark…


10 Proven Ways to Send Nonstop Traffic to Your Webinar Registration Page!
YES - I Want Limitless Traffic!
If you're not completely thrilled with the Limitless Traffic training videos and seeing great results, just email us within 30 days for a complete refund.
The "Limitless Traffic" training videos are the culmination of all my best tactics and tips when it comes to driving high-value, qualified traffic to your webinar registration pages.
The 10 traffic methods you'll discover in this training are not your ordinary "just run ads on Facebook" type strategies.
In fact, I'm all but certain you've never even considered some of the ways I'll reveal to you when it comes to finding (and sending) high-quality, high-value traffic directly to your webinar registration pages.
Using these methods and traffic sources, I regularly send traffic that generates a 40-50 percent signup rate and (even better) a 60-70 show up rate for my webinars.
I've spent the past 5 years honing these traffic sources and methods, and they've proven time and again to deliver incredible results.
I can't wait for you to discover what "Limitless Traffic" has to offer!


Great news! We are a leading Business School in Germany. We, the students, have interesting, international and diverse backgrounds and our professors are well known, committed and passionate.
We can be proud of ourselves! We are prepared for a life on the fast track.
According to the above-mentioned proverb, we would have to go alone. Let's prove the proverb wrong. Let's go fast and far, while having a lot of fun, too. It just makes our exciting journey so much more enjoyable.
A continuously growing number of students requires a continuously growing number of student activities, initiatives and events. There is going be a lot of work for us and a lot to enjoy for you. We'll try to make campus life nothing less than awesome.
And here comes the fun part for you: We need your collaboration. Only together can we sustain and strengthen a group identity as Frankfurt School students. We are happy to say that this is not just a university degree. Our experience on campus constitutes an important and joyful stage of life. And we are here to make that happen!
The Student Council (StuCo) is the connecting link between you and the school and we are involved in major decisions that Frankfurt School takes. We want to be a slight breeze that accompanies student life and we want to be a hurricane when it comes to students' concerns, events and external relationships. We look forward to represent Frankfurt School students, working with you on every project, idea, or problem you might have. The StuCo makes your ideas happen.
We have so many projects in mind already and we want to carry on our predecessors' projects as well. They did a great job!
Look forward to a year full of fun and interesting events. Look forward to a StuCo that is always there. Look forward to another year at Frankfurt School.
If you have any questions, ideas or projects you want to discuss with us, feel free to write us at: exco@fs-stuco.de or visit us during our office hours (Monday & Wednesday: 12.15 – 1.15pm) in the StuCo office on first floor.


text:
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About Fastenal
Over the past 49 years, Fastenal has grown from a small-town fastener shop, to a thriving regional business, to North America's largest fastener distributor, to the world's most efficient supplier of OEM, MRO, and construction products. Along the way, we've never wavered in our belief that great service starts with being close to our customers, which is why today we operate nearly 2,700 branches spanning all 50 states and 20-plus nations.
You'll find Fastenal branches in cities like Houston, Indianapolis, Atlanta, Toronto, and Shanghai. But what really matters is that you'll find a Fastenal branches near you — ready to stock your products, manage your inventory, respond urgently, and provide the kind of customer service you just can't get from a catalog or 1-800 number.
From one store to nearly 2,700 and counting – We Are Where You Are.
The Fastenal story began in 1967 when Bob Kierlin pooled together $30,000 with four friends and opened the first Fastenal store, a 1,000 sq. ft. shop in his hometown of Winona, MN. (The original business plan was to dispense nuts and bolts via custom vending machines, but the technology proved impracticable at the time. Several decades would pass before Fastenal finally popularized industrial vending.)
After surviving the typical struggles of a startup business, Fastenal gradually found its niche – by going the extra mile for customers and providing the kind of service that kept them coming back. Kierlin later drilled this approach down to four simple words: Growth Through Customer Service.
This motto has guided us forward as we've grown from a small regional supplier into one of the world's most dynamic growth companies – from one store to more than 2,600 and counting. Along the way, we've aggressively invested in things that make a difference for our customers, continuously improving a multifaceted service network that today includes:
A stringent quality management system anchored by our engineering teams and testing laboratories around the world.
Thousands of manufacturer-partners, making each Fastenal branch a one-stop source for a huge range of OEM, MRO and Construction products.
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redpajama_set_name: RedPajamaCommonCrawl


text:
Tickets and Boas
WMC Breast Health Center Opens, Focuses on Optimal Patient Care
by Jay Sheridan
(Front left) Matt Largen, president and CEO of Williamson Inc.; Stacie Holloway, CFNP, Williamson Medical Group; Tracy Rogers, RN, Breast Health Center; Julie Miller, WMC Chief Operating Officer; Rebecca Baskin, M.D., Breast Health Surgeon; and Cary Ralph, RN, Breast Health Navigator, (Back left) Rogers Anderson, Williamson County Mayor; Bert Chalfant, WMC Board Member; Jack Walton, WMC Board Member; Paul Bolin, WMC Chief Financial Officer and Starling Evins, M.D., WMC Chief Medical Officer
By Jodi Rall, The Williamson Herald
It was all smiles, and lots of pink, as Williamson, Inc. Chamber members and Williamson Medical Center staff celebrated the opening of the Breast Health Center with a ribbon cutting and open house.
The Breast Health Center, located adjacent to the existing imaging center to allow for more convenient access, is equipped with the latest in 3-D mammography and Tomosynthesis technology.
Staff explained Thursday the team approach to how patients are treated.
Working hand-in-hand, Dr. Rebecca Baskin and her team can offer excellence in patient care focusing on reducing anxiety, and providing peace of mind for women.
Staff explained that if a technician sees a problem during a mammogram, one quick phone call and walk down the hallway is now all that is needed. Women no longer have to wait anxiously for results, and often biopsies can be completed within 24 to 48 hours.
As the primary breast surgeon and breast health specialist, Baskin brings great empathy for her patients as she too once waited for biopsy results. At the age of 36, she was diagnosed with breast cancer. Because of her personal experience, she explained her passion for offering the highest patient care possible.
From Middle Tennessee, Baskin is a board certified surgeon and earned her medical degree from East Tennessee State University in Johnson City, Tn., and did her residency in general surgery at Good Samaritan Hospital in Cincinnati, Ohio.
When Baskin spoke to the crowded room, it was with great emotion. She talked about her husband and family's support.
"I've seen the patient side of it. My family has been beside me," Baskin said.
Working along-side Baskin is Cary Ralph, Breast Health Navigator, RN, CN-BN. Ralph is the first responder of sorts when the imaging center sees a potential problem with a mammography. Her role is to provide comfort and as her title implies, navigate the "what next."
Also, Tracy Rogers, LPN, has been Baskin's long time nurse and is a breast cancer survivor herself.
During the remarks period prior to the ribbon-cutting, Matt Largen, President and CEO of Williamson, Inc. the county's business chamber remarked on the important work the center is doing and complimented Williamson Medical Center as one of the leading employers of the county.
"The Breast Health Center provides peace of mind for patients. Integrated health care with people at the heart of what they do," Largen said.
Julie Miller, Chief Operating Officer WMC, explained, the focus and process.
"We really focus on the patient, the convenience, the mental and physical needs. The patient navigator is available to walk over and talk to a patient whose tests show something abnormal," Miller said.
"Then walk them over to the center. Often times if a biopsy is needed, the procedure will take place within 24-48 hours."
Williamson Medical Group's Breast Health Center has been named one of America's Best Breast Centers for the past two years by the Women's Choice Awards. It is also an NAPBC and Commission on Cancer accredited facility. The Breast Health Center can be reached by calling 615-595-4570.
The Breast Health Center is located at 4601 Carothers Parkway, Suite 150, Franklin, Tennessee.
Mom's Story
Kelly Spalding Designs | 615.442.7662


text:
Tanja Fajon, née le  à Ljubljana, est une femme politique slovène, membre des Sociaux-démocrates.

Biographie

Députée européenne depuis 2009, elle fait partie du groupe Alliance progressiste des socialistes et démocrates au Parlement européen. Elle est membre de la commission des libertés civiles, de la justice et des affaires intérieures.

Elle est pressentie en  pour devenir la commissaire européenne slovène, après que l'ancienne présidente du gouvernement Alenka Bratušek a été recalée par le Parlement européen.

Elle est chef de file et est élue députée aux élections législatives du . Elle démissionne du  Parlement européen le  et est remplacée par Matjaž Nemec.

Notes et références

Voir aussi

Articles connexes
 Liste des députés européens de Slovénie de la  - Liste des députés européens de la
 Liste des députés européens de Slovénie de la  - Liste des députés européens de la
 Liste des députés européens de Slovénie de la  - Liste des députés européens de la

Liens externes

Femme politique slovène
Personnalité des Sociaux-démocrates (Slovénie)
Femme ministre slovène
Ministre slovène des Affaires étrangères
Député européen membre des Sociaux-démocrates (Slovénie)
Député européen du groupe Alliance progressiste des socialistes et démocrates au Parlement européen 2019-2024
Député européen élu en Slovénie 2019-2024
Député européen du groupe Alliance progressiste des socialistes et démocrates au Parlement européen 2014-2019
Député européen élu en Slovénie 2014-2019
Député européen du groupe Alliance progressiste des socialistes et démocrates au Parlement européen 2009-2014
Député européen élu en Slovénie 2009-2014
Naissance en mai 1971
Naissance à Ljubljana

redpajama_set_name: RedPajamaWikipedia


In a very special July issue (out now), Hugo Shirley reappraises Herbert von Karajan's landmark recordings of Wagner's Ring cycle, which began with the release of Das Rheingold 50 years ago. In an engrossing article, Shirley speaks to Gundula Janowitz (who appeared on the Die Walküre and Götterdämmerung recordings) and others about the project and reflects on how Karajan's Ring compares to Georg Solti's earlier, more famous, cycle.
Here on the Gramophone website, we've gathered a host of articles, including the full original reviews from 1967 to 1970, and profiles and interviews with the principal artists, for you to explore this most ambitious of recording projects.
Plus, we have a very special offer for our readers from the Berlin Philharmonic's Digital Concert Hall, and don't miss our competition to win one of two copies of the newly remastered Karajan Ring cycle on Blu-ray Audio, courtesy of DG. Enjoy!


text:
El condado de Fremont (en inglés: Fremont County), fundado en 1893, es uno de los 44 condados del estado estadounidense de Idaho. En el año 2000 tenía una población de 11 819 habitantes con una densidad poblacional de 2.4 personas por km². La sede del condado es St. Anthony.

Geografía
Según la Oficina del Censo, el condado tiene un área total de , de la cual  es tierra y  (1.52%) es agua.

Condados adyacentes
 Condado de Clark - oeste
 Condado de Jefferson - suroeste
 Condado de Madison - sur
 Condado de Teton - sur
 Condado de Teton - este
 Condado de Gallatin - norte
 Condado de Madison (Montana) - norte
 Condado de Beaverhead - noroeste

Demografía
En el 2000 la renta per cápita promedia del condado era de $$33 424, y el ingreso promedio para una familia era de $36 715. En 2000 los hombres tenían un ingreso per cápita de $26 490 versus $19 670 para las mujeres. El ingreso per cápita para el condado era de $13 965. Alrededor del 14.20% de la población estaba bajo el umbral de pobreza nacional.

Comunidades

Ciudades
 Ashton
 Drummond
 Island Park
 Newdale
 Parker
 St. Anthony
 Teton
 Warm River

Otras comunidades
 Big Springs
 Chester
 Lake
 Macks Inn
 Squirrel

Referencias

Enlaces externos

 Web del condado
 Fremont County Joint School District 215


text:
Reebok Addresses That Beyoncé Rumor
Reebok Addresses That Beyoncé Rumor About The Lack of Diversity
Photo: Kevin Winter/Getty Images.
Update #2, April 8: Reebok addressed the rumor that Beyonce decided not to work with the company due to a lack of diversity in the following statement to Refinery29:
"The report that Beyoncé walked out of a meeting with Reebok due to lack of diversity is categorically false. Our discussions with Beyoncé and her team continued for several months after our initial meeting. We are disappointed that false information is being reported as fact."
Update: In a recent episode of ESPN's "The Jump," writer Nick DePaula said Beyonce was previously in talks with Reebok about a potential partnership. He claims she opted out of working with the sneaker brand because of the pitch team's lack of diversity.
"She had a meeting at Reebok and they had a whole presentation of everything, potential products, how this could all look," he explained, "and she kinda took a step back and said 'is this the team that would be working on my product'? And somebody said 'yes' and she said 'nobody in this room reflects my background, my skin color, and where I'm from and what I want to do'. And so she kinda took a step back and left and then, it did not come to terms."
ESPN Writer @NickDePaula reveals Beyoncé walked out of a meeting w/ @Reebok after she highlighted the pitch team's lack of diversity & non-existent representation of her background and skin color. ?
He also talks about Bey getting offers from Jordan (@Jumpman23) & @UnderArmour. pic.twitter.com/J2P3cvGw6I
— BEYONCÉ LEGION (@BeyLegion) April 5, 2019
According to DePaula, she also had discussions with Under Armour and Jordan Brand as well, but ultimately, she decided to move forward with Adidas.
This story was originally published on April 4, 2019.
Beyoncé is joining the Adidas family, which already includes a familiar face, Kanye West and his infamous Yeezys. On Thursday, Adidas announced a new "multi-layered partnership" with the Lemonade singer that will include inspiring and empowering the next generation of creators, driving positive change in the world through sport, and identifying new business opportunities, according to a release.
"This is the partnership of a lifetime for me," Beyoncé said in the same release. "Adidas has had tremendous success in pushing creative boundaries. We share a philosophy that puts creativity, growth and social responsibility at the forefront of business. I look forward to re-launching and expanding Ivy Park on a truly global scale with a proven, dynamic leader."
The new Ivy Park will include exciting products in the athleisure space that focus on empowering and enabling the next generation of athletes, creators and leaders. And because it's Beyoncé, we can expect rich storytelling and graphics.
"As the creator sports brand, Adidas challenges the status quo and pushes the limits of creativity through its open source approach," Eric Liedtke, Executive Board Member - Global Brands, Adidas
said in a press release. "Beyoncé is an iconic creator but also a proven business leader, and together, we have the ability to inspire change and empower the next generation of creators."
Last year, Beyoncé bought back Ivy Park, her athleisure line, from Topshop after mogul Philip Green's alleged sexual harassment case. Her new partnership with Adidas will respect Beyoncé's full ownership of Ivy Park which continues her journey as one of the first black women to be the sole owner of an athleisure brand.
Beyonce Bought Back Ivy Park, Relaunches With Adidas
Fashion • Adidas • Beyonce • Celebrity Style • Designers


This example shows how to use the standard XSL Transformations to transform an XML file into VoiceXML and HTML. It demonstrates the use of Perl and Microsoft's Active Server Pages to load XML documents and XSLT stylesheets.
XSL Transformations are ideal for purposing raw data into a variety of output formats including HTML, VoiceXML, and print. Alternatively, you can use the data element to load the XML directly from a static VoiceXML document.
An XSLT stylesheet is used to transform an existing XML file into the desired format (VoiceXML or HTML) The default output format is VoiceXML, the format that the Tellme voice browser parses and executes. The server side script loads both the XML document and the specified XSLT document to perform the transformation.
The Tellme developer data set in this sample is loaded from a static XML file. You can easily write a CGI script to pull data from a database and to reformat that data as XML that your XSLT can transform.
The following XSLT stylesheet is used to transform the sample data set shown above into VoiceXML 2.0 format.
The following XSLT stylesheet is used to transform the sample data set shown above into HTML format.
The following Perl script is used to load the XML data set and one of the XSLT stylesheets to produce the desired output. To run this script on your own Web server, you'll need to make sure that Perl is installed in addition to the XML::XSLT and Perl CGI modules.
#Copyright (C) 2000-2001 Tellme Networks, Inc. All Rights Reserved.
# Search the Web for other XSLT processors.
The following Active Server page is used to load the XML data set and one of the XSLT stylesheets to produce the desired output. To run this code, you'll need to save it to a server running Windows 2000 or later and Microsoft's XML parser version 3.0 or later.


text:
ELECTRON TRANSPORT IN AND ELECTROCATALYSIS WITH POLYMERIC FILMS OF METALLOTETRAPHENYLPORPHYRINS.
Royce W. Murray, B. A. White, A. Bettelheim
Amino-, hydroxy-, and pyrrole-substituted tetraphenylporphyrins undergo electrooxidative polymerizations analogous to those of aniline, phenol, and pyrrole, to form electroactive poly-porphyrin films on electrode surfaces. The voltammetry of a number of differently metallated forms of the poly-porphyrins has been studied as has the rate of electron-hopping diffusion within the polymers. The electron mobilities form a parallel to heterogenous electron transfer rate constants for corresponding metalloporphyrin monomers at solid electrode surfaces, consistent with lack of dominance of ionic or polymer chain motions on the barrier to electron transfers within the poly-porphyrin films. Films of the cobalt-metallated poly-porphyrins exhibit electrocatalytic activity toward reduction of dioxygen both in solutions and in the solid state.
Polymeric Materials Science and Engineering, Proceedings of the ACS Division of Polymeric Material
Dive into the research topics of 'ELECTRON TRANSPORT IN AND ELECTROCATALYSIS WITH POLYMERIC FILMS OF METALLOTETRAPHENYLPORPHYRINS.'. Together they form a unique fingerprint.
Electrocatalysis Engineering & Materials Science 100%
Porphyrins Engineering & Materials Science 96%
Electron Transport Engineering & Materials Science 87%
Polymer films Engineering & Materials Science 72%
Electrons Engineering & Materials Science 41%
Liquid Film Chemical Compounds 26%
Electron Transfer Chemical Compounds 25%
Tetraphenylporphyrin Chemical Compounds 22%
Murray, R. W., White, B. A., & Bettelheim, A. (1987). ELECTRON TRANSPORT IN AND ELECTROCATALYSIS WITH POLYMERIC FILMS OF METALLOTETRAPHENYLPORPHYRINS. In Polymeric Materials Science and Engineering, Proceedings of the ACS Division of Polymeric Material (pp. 864). (Polymeric Materials Science and Engineering, Proceedings of the ACS Division of Polymeric Material; Vol. 56). ACS.
Murray, Royce W. ; White, B. A. ; Bettelheim, A. / ELECTRON TRANSPORT IN AND ELECTROCATALYSIS WITH POLYMERIC FILMS OF METALLOTETRAPHENYLPORPHYRINS. Polymeric Materials Science and Engineering, Proceedings of the ACS Division of Polymeric Material. ACS, 1987. pp. 864 (Polymeric Materials Science and Engineering, Proceedings of the ACS Division of Polymeric Material).
@inproceedings{8a7a345443584b9ea2850ea976f9d627,
title = "ELECTRON TRANSPORT IN AND ELECTROCATALYSIS WITH POLYMERIC FILMS OF METALLOTETRAPHENYLPORPHYRINS.",
abstract = "Amino-, hydroxy-, and pyrrole-substituted tetraphenylporphyrins undergo electrooxidative polymerizations analogous to those of aniline, phenol, and pyrrole, to form electroactive poly-porphyrin films on electrode surfaces. The voltammetry of a number of differently metallated forms of the poly-porphyrins has been studied as has the rate of electron-hopping diffusion within the polymers. The electron mobilities form a parallel to heterogenous electron transfer rate constants for corresponding metalloporphyrin monomers at solid electrode surfaces, consistent with lack of dominance of ionic or polymer chain motions on the barrier to electron transfers within the poly-porphyrin films. Films of the cobalt-metallated poly-porphyrins exhibit electrocatalytic activity toward reduction of dioxygen both in solutions and in the solid state.",
author = "Murray, {Royce W.} and White, {B. A.} and A. Bettelheim",
series = "Polymeric Materials Science and Engineering, Proceedings of the ACS Division of Polymeric Material",
publisher = "ACS",
booktitle = "Polymeric Materials Science and Engineering, Proceedings of the ACS Division of Polymeric Material",
Murray, RW, White, BA & Bettelheim, A 1987, ELECTRON TRANSPORT IN AND ELECTROCATALYSIS WITH POLYMERIC FILMS OF METALLOTETRAPHENYLPORPHYRINS. in Polymeric Materials Science and Engineering, Proceedings of the ACS Division of Polymeric Material. Polymeric Materials Science and Engineering, Proceedings of the ACS Division of Polymeric Material, vol. 56, ACS, pp. 864.
ELECTRON TRANSPORT IN AND ELECTROCATALYSIS WITH POLYMERIC FILMS OF METALLOTETRAPHENYLPORPHYRINS. / Murray, Royce W.; White, B. A.; Bettelheim, A.
Polymeric Materials Science and Engineering, Proceedings of the ACS Division of Polymeric Material. ACS, 1987. p. 864 (Polymeric Materials Science and Engineering, Proceedings of the ACS Division of Polymeric Material; Vol. 56).
T1 - ELECTRON TRANSPORT IN AND ELECTROCATALYSIS WITH POLYMERIC FILMS OF METALLOTETRAPHENYLPORPHYRINS.
AU - Murray, Royce W.
AU - White, B. A.
AU - Bettelheim, A.
N2 - Amino-, hydroxy-, and pyrrole-substituted tetraphenylporphyrins undergo electrooxidative polymerizations analogous to those of aniline, phenol, and pyrrole, to form electroactive poly-porphyrin films on electrode surfaces. The voltammetry of a number of differently metallated forms of the poly-porphyrins has been studied as has the rate of electron-hopping diffusion within the polymers. The electron mobilities form a parallel to heterogenous electron transfer rate constants for corresponding metalloporphyrin monomers at solid electrode surfaces, consistent with lack of dominance of ionic or polymer chain motions on the barrier to electron transfers within the poly-porphyrin films. Films of the cobalt-metallated poly-porphyrins exhibit electrocatalytic activity toward reduction of dioxygen both in solutions and in the solid state.
AB - Amino-, hydroxy-, and pyrrole-substituted tetraphenylporphyrins undergo electrooxidative polymerizations analogous to those of aniline, phenol, and pyrrole, to form electroactive poly-porphyrin films on electrode surfaces. The voltammetry of a number of differently metallated forms of the poly-porphyrins has been studied as has the rate of electron-hopping diffusion within the polymers. The electron mobilities form a parallel to heterogenous electron transfer rate constants for corresponding metalloporphyrin monomers at solid electrode surfaces, consistent with lack of dominance of ionic or polymer chain motions on the barrier to electron transfers within the poly-porphyrin films. Films of the cobalt-metallated poly-porphyrins exhibit electrocatalytic activity toward reduction of dioxygen both in solutions and in the solid state.
T3 - Polymeric Materials Science and Engineering, Proceedings of the ACS Division of Polymeric Material
BT - Polymeric Materials Science and Engineering, Proceedings of the ACS Division of Polymeric Material
PB - ACS
Murray RW, White BA, Bettelheim A. ELECTRON TRANSPORT IN AND ELECTROCATALYSIS WITH POLYMERIC FILMS OF METALLOTETRAPHENYLPORPHYRINS. In Polymeric Materials Science and Engineering, Proceedings of the ACS Division of Polymeric Material. ACS. 1987. p. 864. (Polymeric Materials Science and Engineering, Proceedings of the ACS Division of Polymeric Material).


text:
Wikimujeres
This Wikimedia movement affiliate is a member of Iberocoop
Wikimujeres Grupo de Usuarias is a recognised Wikimedia user group for women and allies in the wiki movement. Working language is Spanish.
ObjectivesEdit
Support efforts to increase content and contributor diversity on Wikimedia projects, with a focus on Spanish-speaking ones
Organize offline activities such as meetups and conferences about gender diversity
¿Qué es una editatona? ¿Porqué es importante trabajar con perspectiva de género en Wikpedia? El reto de superar la brecha de género en la enciclopedia más usada del mundo.Cármen Alcázar de Wikimedia México y Wikimujeres nos lo cuenta. Rodado en Esino Lario. Wikimanía 2016
ActivitiesEdit
EditathonAs
Collaborations with other orgs
ReportsEdit
Please check here.
ContactEdit
For any information please contact us at the talkpage or write directly to esterbonet@gmail.com; info@wikimujeres.wiki
You can also check what we are up to on Twitter.
Ester Bonet Wikimujeres: an international women's movement on wikipedia (català)
Contacts declared to WMFEdit
Tiputini (Primary contact)
Mboix (Secondary contact)
Interested in participatingEdit
Wikimujeres in Wikipedia15th anniversary party in Madrid
en: Please sign you name below by by clicking 'edit' and adding *~~~~ to the bottom of the list.
es: Por favor, introduce tu nombre debajo. Haz clic en "editar" y añade
Raystorm (talk) 16:40, 8 October 2015 (UTC)
Olgaberrios (talk) 16:44, 8 October 2015 (UTC)
Mboix (talk) 16:44, 8 October 2015 (UTC)
Rosiestep (talk) 14:43, 9 October 2015 (UTC)
Fluffernutter (talk) 16:07, 11 November 2015 (UTC)
Sydney Poore/FloNight (talk) 16:31, 11 November 2015 (UTC)
Jaluj (talk) 15:15, 13 November 2015 (UTC)
Tiputini (talk) 21:44, 28 December 2015 (UTC)
SinAcritud (talk) 16 Febrero 2016
Misabel.menendez (talk) 16 Febrero 2016
MAuxiJiménez16 Febrero 2016
Maviliña (talk) 16 Febrero 2016
Emelinica(talk) 18 de febrero
GDuarteAbós (talk) 12:15, 18 Febrero 2016 (UTC)
Mentxuwiki (talk) 17:36, 19 February 2016 (UTC)
VivianIsidora (talk) 21 Febrero 2016 (UTC)
EdurneR (talk) 7 Marzo 2016 (UTC)
PatriHorrillo (talk) 19:52, 18 March 2016 (UTC)
Maríajoséblanco (talk) 16:13, 20 March 2016 (UTC)
Maitelirona (talk) 27 de marzo 2016
Señoritaleona (talk) 22:37, 12 April 2016 (UTC)
Yolanda lalonso artista (talk) 17:33, 9 May 2016 (UTC)
Gollimart (talk) 12:56, 5 July 2016 (UTC)
Luz Maria Utrera (talk) 19:24, 12 August 2016 (UTC)
NitalaPansera (talk) 14:32, 26 September 2016 (UTC)
ClaraPao (talk) 18:40, 9 January 2017 (UTC)
VickyBayVi (talk) 19:28, 9 January 2017 (UTC)
Marisa Padilla Esteban (talk) 19:42, 9 January 2017 (UTC)
AsorB (talk) 19:19, 23 January 2017 (UTC)
Nekkena (talk) 19:52, 23 January 2017 (UTC)
Wotancito (talk) 02:18, 27 January 2017 (UTC)
Moniquiña (talk) 19:03, 27 February 2017 (UTC)
Valle ramos (talk) 19:07, 27 February 2017 (UTC)
GoboFR (talk) 19:30, 27 February 2017 (UTC)
Greta Mencart (talk) 18:32, 6 March 2017 (UTC)
Teresa Alario (talk) 18:21, 7 March 2017 (UTC)
MJPVILLARINO (talk) 18:21, 7 March 2017 (UTC)
Angelicavs (talk) 18:23, 7 March 2017 (UTC)
Verónica55 (talk) 18:24, 7 March 2017 (UTC)
Ivansambade (talk) 18:26, 7 March 2017 (UTC)
AndreaGBC (talk) 18:27, 7 March 2017 (UTC)
Tatianapsa (talk) 18:28, 7 March 2017 (UTC)
Fcruzsouza (talk) 18:29, 7 March 2017 (UTC)
Paula Cancio (talk) 18:30, 7 March 2017 (UTC)
Cnualart (talk) 17:42, 27 March 2017 (UTC)
Trotwood74 (talk) 17:46, 27 March 2017 (UTC)
Mariettajgarcia (talk) 17:49, 27 March 2017 (UTC)
Pablísima (talk) 21:59, 1 April 2017 (UTC)
Alimacbil (talk) 16:13, 14 April 2017 (UTC)
Gini10 (talk) 11:44, 19 August 2017 (UTC)
Caleidoscopic (talk) 17:06, 15 January 2018 (UTC)
Escalafandra (talk) 19:03, 29 January 2018 (UTC)
Escierzo (talk) 11:04, 30 January 2018 (UTC)
Yhhue91 (talk) 17:11, 10 February 2018 (UTC)
Camelia (talk) 19:50, 24 February 2018 (UTC)
Lizalamandra (talk) 15:40, 03 March 2018 (UTC)
Nat2000 (talk) 11:31, 5 March 2018 (UTC)
John Cummings (talk) 11:31, 5 March 2018 (UTC)
Fpasquale (talk) 11:31, 8 March 2018 (UTC)
Severincarminati (talk) 11:31, 8 March 2018 (UTC)
Beatrizpalacios (talk) 20:11, 8 March 2018 (UTC)
l_valkyrie (talk) 16:44, 8 March 2018 (UTC)
Pintakuda (talk) 17:59, 12 March 2018 (UTC)
John Cummings (talk) 11:31, 5 March 2018 (UTC) al final de la lista.
rosaritafe
Celia Antonina Hernández (talk) 18:23, 19 March 2018 (UTC)
Elenaib (talk) 19:24, 19 March 2018 (UTC)
--XanaIgle (talk) 09:23, 24 March 2018 (UTC)
--Paux33rf (talk) 09:24, 24 March 2018 (UTC)
--Patriciamf84 (talk)
Sanmon86 (talk) 08:47, 3 April 2018 (UTC)
TitiNicola (talk) 23:32, 21 April 2018 (UTC)
--Diana Zavalza (talk) 15:23, 08 May 2018 (UTC)
--Melissamarzo (talk) 16:14, 13 December 2018 (UTC)
--MyraLeeVzla (talk)
*~~~~
ResolutionsEdit
Recognition Wikimujeres Grupo de Usarias - November 2015
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This post was written by Brian Handerhan, business development manager with Parker Hannifin's life science automation group.
We have all heard that the Baby Boomers are marching toward retirement, and we have questioned how that will affect healthcare costs and society in general. In the life sciences in particular, however, we know this generation will influence the use of—and need for—robotics in clinical, diagnostic, and pharmacological laboratories.
The 60-year-old-plus population uses three-to-five times the healthcare services that younger generations use. That group is expected to grow by 33 percent between 2010 and 2020. Furthermore, that population is expected to jump from 18 percent of the total population to 22 percent in that 10-year span, according to the Administration for Community Living, U.S. Department of Health and Human Services.
With that growing population demanding the lion's share of healthcare, the volume of clinical and diagnostic testing will increase dramatically, straining the capability of laboratories and their staffs. Additionally, the growing demand to develop new drugs to treat the patient pool will fuel capacity expansion in drug discovery.
The pressure to contain healthcare costs has been increasing, and the changing demographics will likely drive up that containment pressure exponentially. This takes automation from a "nice to have" to a "must do." Laboratory robotics offers the promise of increased efficiencies, improved throughput times, and reduced costs, much as the moving assembly line did for Henry Ford in the automobile industry. And as the demand for new drugs to treat the aging population skyrockets, robotics will help the drug discovery process keep pace through around-the-clock research.
Before such automation, scientists were hampered by manual testing. Today's automated high-throughput screening empowers scientists with access to an abundance of data—with little or no manual interaction.
The engines behind automation's faster pace are higher throughput machines powered by servomotors. Stepper motors have been the technology of choice since the inception of the laboratory automation space, and although they continue to be the correct solution for many applications, more applications are requiring the greater speeds and high dynamic response of servos.
Many instrument manufacturers are also replacing mechanical drive trains with linear motors in robotics and other automation. They have superior smoothness and accuracy while enabling higher speed, lower maintenance, less down time, precision performance, and longer overall life. For example, new compact motors are often integrated into centrifuges and instruments requiring a very small footprint, as they can be built right into the machine.
The increasing volume of testing and the specificity of tests require equipment that takes up less room. That is why standard positioning devices are getting smaller. In fact, the overall footprint of standard motion products continues to shrink in an effort to provide solutions to original equipment manufacturers (OEMs) as they shrink their instrument sizes.
Where the form factor of standard products does not fit this new world, customized actuators can also be integrated into instruments. Solutions are still being engineered to fit directly into existing instruments to serve as the structure of the motion system where it makes sense.
Personalized medicine itself is a megatrend that is at the intersection of a number of major technology trends. According to Wikipedia, personalized medicine is a "medical model that proposes the customization of healthcare—with medical decisions, practices, and/or products being tailored to the individual patient." Personalized medicine employs genetic testing to help select the most appropriate therapy based on the genetic makeup of the patient.
The cost of sequencing an individual's genetic code is continuing to decrease and is now approaching $1,000 U.S. That cost brings new developments in sequencing ribonucleic acid (RNA), allowing doctors to better differentiate external environmental impacts on health from individual genetic tendencies. This gives a better perspective on the individual's overall health. It is becoming possible to understand an individual's genetic makeup, so that responsiveness to certain drugs and therapies can be predicted, allowing the best individualized care.
"Big data" refers to the collection and use of data sets that are so large that just a few years ago, they were impossible to manage with traditional computing and data processing applications. The collection and application of decoded genetics fits into this definition, and in fact, data management has been a factor in the cost and commercial viability of this tool.
Big data has also facilitated collecting huge numbers of test samples during the drug discovery process, allowing a real understanding of how drugs will perform given a genetic disposition. Coupled with a high level of automation in the testing process, the number of iterative samples is growing exponentially.
The real benefits of patient-specific cellular therapies have not yet progressed beyond experimental trials, but they are showing such great promise that it is difficult not to get excited about how they could transform medicine.
According to James Price, the president and chief executive of the Canadian Stem Cell Foundation, stem cell therapy will transform health care and how we treat devastating diseases. "We are on the verge of breakthroughs that will fundamentally alter the treatment of illnesses such as diabetes, cancer, heart disease, and neurological diseases," he believes.
Because manufacture of patient-specific cellular therapies is a discrete process compared to the batch manufacturing processes typically employed in the pharmaceutical manufacturing environment, it will drive a mindset change from "scale up" (increase batch sizes) to "scale out" (increase capacity at the bottleneck).
Big data capabilities and personalized medicine technologies require laboratories to operate 24 hours per day, seven days per week.
Automation of previously manual operations is a major factor driving down the cost of personalized medicine to the point where it is commercially viable for the masses.
With greater use of the tool, drug companies will continue to accelerate their testing to develop drugs that are proven for given genetic dispositions.
Modularity and scalability really mean lean automation. In this approach, instruments run unattended with some level of operator load and unload. This minimizes capital costs. Increasing capacity is a simple matter of adding another instrument to the system.
With requirements to run around the clock in remote locations that do not typically have the on-site maintenance teams many factories have, mean time between failure is critical in today's laboratory robotics. Using industry-proven designs with thousands of hours of operation greatly reduces the risks associated with a new design.
Selectable levels of integration allow designers to choose robust standard products or highly value-added system-level solutions to reduce risk and accelerate development.
More and more instrument OEMs are choosing to outsource some or all of their instrument design and manufacturing. That is because during the "Great Recession," many organizations cut deeply into their engineering talent. Today, in the spirit of a jobless recovery, they have turned to outsourcing as a tool to get products released.
Increasingly, speed to market is a major factor in their success, and outsourcing either the entire design or key subsystems allows more resources to be applied for a shorter design cycle. In fact, it is becoming more common for the majority of an OEM's revenue to come from sales of the consumable as opposed to sales of the instrument. This is why OEM innovation is now more focused on developing revenue-generating consumables.
OEMs must now choose how they define their core competency and what they want to outsource. The answers range from outsourcing just the design to outsourcing just the manufacturing to all options in between. If an OEM chooses to maintain control over the system-level design, it typically wants suppliers with engineering capabilities to do submodule design. By sourcing modular subsystems from a trusted supplier, companies can ensure they get fully qualified, plug-in systems that reduce the overall risk throughout the life cycle of the instrument.
There is a greater physical separation between OEM design teams and OEM manufacturing teams, whether for geographical or organizational reasons. That is why it is critical to have a partner who operates as an extension of the instrument development team. This reduces the OEM's overall engineering resource requirement. With more manufacturing moving to offshore contract manufacturers, the ideal partner should be able to engineer where the OEM is engineering and manufacture where the OEM is manufacturing.
Powerful market forces are driving exciting changes in the use and design of laboratory automation and robotics. New technologies will change healthcare as we know it, bringing costs down to a point of widespread viability. The instrument manufacturers in this space are having to reduce their development cycles, improve their product capabilities, and increase their overall reliability. Moreover, they are relying more on partners to help them achieve their goals. Ideally, these automation partners will provide them with a portfolio of robust standard products for rapid early development efforts, the engineering capabilities to add value, technologies to optimize the product design for specific applications, and the overall process capability to act as an extension of the OEM's team both in development and production.
Brian Handerhan is a business development manager focusing on Parker Hannafin's life science automation group. Handerhan has more than 20 years of experience in the implementation of automation across a broad range of industries. His primary expertise has been as a process improvement leader, change agent, and P&L owner. He now focuses on working with industry OEMs to develop lasting business relationships built on operational and technical value.


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Why hello May (ok, it's more like the end of April, but anyway)!
No need for me to remind us all, including myself, that we should be well into the challenge by now, right? Focus on your chosen level, then add up the books you've read for it, and unless you can't claim to have read a third of the tomes needed, well ... what are you waiting for?
Myself, I am still sitting quite comfy on the first level, and with two more heavy books (or one super-tome, I really haven't decided just yet) to go for the next level, I can actually relax a wee bit longer. Of course by summer I really want to get started on finishing the rest of the books I need, but until then I am doing my best impression of a lazy bum. I might keep on drinking tea though. Not as though that would count in the challenge, but oh well.
In case you've been wondering - yes, you may still sign up for the challenge and get acquainted with the general rules over HERE. In case you already read a tome that qualifies for this challenge during the first part of 2013, that book will of course count towards your chosen level.
Updates for the challenge will be posted regularly on Sundays near the end/beginning of a month and the next dates will thus be June 2nd, and June 30th.
Have you been just as lazy as yours truly or did you get some heavy tome read this month? Please share!
I am half way done (easy enough when I only committed to 2 books!). I have a rule question: I am considering a biography of Eleanor Roosevelt which was published in 2 volumes. Each volume is just over 500 pages. If I read both volumes does that count as one book toward this challenge?
Good question - the answer is, yes!
It's not cheating, especially if it works for you. In fact, as Geoff pointed out below, it seems to be quite a smart move!
I've finished two of my selected books and read an additional book so I'm at 50% of my expected with an extra book on top. So with my remaining two books, Les Miserables being well over the 1200 mark, I should bump up to the Earl Gray Aficionado level which is good because I prefer Earl Gray!
Wallowing ... you see right through me, Geoff! And I must admit, I prefer Earl Grey too, so when I'm done with this wallowing-thing, maybe I will get my British tea time treat too.
I am halfway, and read the first book of the two I was going to do. Anna Karenina is in the version I read 935 pages long. I read this book for another challange as well, but that is allright, isn't it?
Good to see others made progress as well!
I will try t read my other book during the Summer holidays, plenty of time then.
Books read for this challenge may absolutely cross over with other challenges!
I'm three-quarters of the way to the Berry Tea Level, with 3 books read. I finished the last book during the first week of April, so it's time I started another - maybe one of my non-fiction tomes, so that would count towards the This Isn't Fiction challenge as well. I'm not doing very well with that one!
Reading books that qualify for both challenges, now that's smart! I don't think I own any non--fiction tomes though, darn it!
This month I read 2 big books. The Other Boleyn Girl with 672 and Angels & Demons with 713 pages. Still need 2 more books this year to meet my goal for the Earl Grey level but I have them lined up already!!
That tea sounds delicious and yes, reading the commentaries definitely counts towards the 650+ pages needed.


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Thank you for your interest in Fuel. Please feel free to reach out to us with any questions, comments or interest in getting involved.


text:
Deepfakes a growing problem: Experts
ST, 26 Jun 2019, Deepfakes a growing problem: Experts
They call for greater awareness as tech used to create fake videos becomes more easily available
Deepfake videos created using face-swopping technology are challenging the notion that seeing is believing, with experts saying that the problem is bigger than ever and calling for greater awareness about digital trickery.
Celebrities, politicians and everyday people have all been targeted in the videos, while a gay sex video purportedly featuring Malaysia's Economic Affairs Minister Azmin Ali is currently being scrutinised to see if it has been faked.
Algorithms in deepfake videos look for instances where the expressions of individuals whose faces are being synthesised show similar expressions and facial positioning.
After finding the best match through a machine learning process called "generative adversarial networks", the faces are swopped.
Information about the technology is publicly available and the ability to generate them is spreading, with a Google search showing anyone can pay someone else to create a deepfake video.
For example deepfakesweb.com charges just $10 to create a video, which can be ready in four hours.
Mr Bryan Tan, a lawyer from Pinsent Masons MPillay specialising in technology law and data protection, said the problem has been around for about six years and is getting worse. "With such easy availability and usability, mass use of this becomes a danger especially to an unsuspecting public," he said.
A spokesman for cyber security company Malwarebytes Labs told The Straits Times that the phrase "deepfake" was coined in 2017, when a Reddit user with the handle DeepFakes posted explicit videos of "celebrities", whose faces replaced those of pornographic actors.
Since then, the technology has improved vastly.
"With the recently developed software and hardware, creating a deepfake video is so easy that the hardest part is to find enough still images to feed to the algorithm in order to create a realistic imitation," said the spokesman.
"If we have the original video of a person giving a speech, we only need to type out the text we want them to say to change the existing video into the desired one."
Tell-tale signs of a deepfake video, the firm says, are a distorted background or unnatural and asymmetrical facial features. But it warned that forensic tools to spot deepfake videos now only focus on certain characteristics which could easily be avoided by malicious actors.
Yet even fake videos that are not well produced can still become popular. Last month, a distorted video depicting US House Speaker Nancy Pelosi with slurred speech and acting drunkenly showed how even basic manipulation can trick its way into being shared by many.
The head of the humanities, arts and social sciences at Singapore University of Technology and Design, Professor Lim Sun Sun, explained that the appeal of deepfake videos lies in their emotional appeal.
"When something has that shock value it makes you sit up, it makes you even want to share it," said the Nominated MP and Media Literacy Council (MLC) member. "It is a kind of a psychological bias that we are all predisposed to."
That is why when educating the public about fake news, she said, the MLC reminds people to be alert to any kind of content that seems extreme in nature, as reactions like anger, disgust or even sympathy could encourage people to share the content without first assessing its validity.
Mr Tan said that while many videos are still legitimate and netizens "still have reason to trust photos and video", the rise in deepfakes and their ease of creation means that netizens must treat the content they consume critically rather than blindly accepting it.
Prof Lim advises that before sharing unusual content, individuals should check with relevant parties or individuals first, and compare the information to another source.
"We need to be more circumspect and less gullible, to recognise and internalise the fact that there are increasingly fake news purveyors out there, operating at extremely high levels of sophistication," she said. "So any kind of news or content that seems too extreme or too sensationalist should be taken with a pinch of salt, and we should all do the due diligence to find out more before we seek to comment or to share."
TECHNIQUES USED TO CREATE FAKE VIDEOS
FACE SWOP
Many people might be familiar with this in Instagram and Snapchat filters, but such technology - which uses an algorithm to seamlessly insert the entire face of a person onto another - can be dangerous. This technique could put people in situations they were never really in by placing their face onto another person's body.
FACIAL REENACTMENT
This technique can transfer facial expressions onto a person in another video - no matter what his appearance - making him appear angry, surprised or disgusted.
Grafting a lip-syncing mouth onto the mouth of someone else and combining the footage with audio can make it seem like a person is saying something he never said.
MOTION TRANSFER
This advanced form of deepfake video captures the movements of a person and transfers them to another target. According to Nieman Lab at Harvard, Wall Street Journal correspondent Jason Bellini, working with researchers at the University of California, Berkeley, tried this technique out for himself and ended up dancing like Bruno Mars.
YANG MI, FEBRUARY 2019
The problem of deepfake videos was thrust into the national spotlight in China when the face of well-known actress Yang Mi, 32, was spliced onto a television drama that aired 25 years earlier.
The face of actress Athena Chu was replaced with Yang Mi's, causing hilarity – and concern – on social media.
It became one of the top trending stories on Weibo, with the related hashtag being read over 120 million times.
The incident prompted China's top legislative body to raise concerns about deepfake videos and artificial intelligence technology.
KIM KARDASHIAN WEST, MAY 2019
On May 29, anti-advertising activists Brandalism uploaded a fake but realistic video of reality star Kim Kardashian West to YouTube.
She was depicted discussing a shadowy organisation called "Spectre" and mocking her fans for violating copyright. The video used to make this deepfake was uploaded in April by Vogue magazine.
The magazine's publisher, Conde Nast, made a copyright claim to the video, and YouTube has since removed it.
KIT HARINGTON, JUNE 2019
A deepfake video of Game Of Thrones main character Jon Snow apologising for the show's polarising final season went viral earlier this month.
According to the New York Post, the video titled "Breaking: Jon Snow finally apologised for Season 8" was posted by YouTube channel Eating Things on June 13 and amassed more than 1.7 million views.
In the video, Kit Harington, who plays Jon, refers to how a coffee cup was accidentally left on a table in the season's fourth episode of the final season. He also "apologised" for the season's conclusion, saying: "I know nothing made sense at the end."


While google-reading lately, I came across several mentions of Cammie (Carolyn King)'s efforts to host a challenge to benefit something that is very dear to her. So I checked it out, and she has asked for all who participate to please send a thank you to someone who cares for Alzheimers patients. Please see this post for details. A lot of companies and individuals have donated approx. $1000 in products for the random lucky winner that posts the card he/she sent for this cause. I am glad to be able to participate in this challenge - I know how very difficult it is to be a caregiver!
So here's my very simple card that will be sent off to hopefully brighten someone's day by letting them know they are appreciated! Will you join this cause?
Excellent card! It's a true Becky original!
That's so awesome of you to do this! Love the card too, the star is fantastic!
you sure do know how much goes into being a caregiver, I think you deserve your own card! love this Becky-you do wonders with those stars! great one.


Sean, an imaginative, soccer-loving second grader, wants to be the great Leo Messi, and he's working hard to accomplish his goal. He battles fears, bullies, nagging parents, and tiresome teachers in pursuit of his dream to become the best soccer player in the world.
An engaging, relatable children's book about soccer, practice, and inspiration.
Beautiful illustrations by Elettra Cudignotto.


Legacy League's Annual Christmas Home Tour showcases five extraordinary homes, ranging from traditional to contemporary.
Launched in 2011, Samford Legacy League's Christmas Home Tour has become a beloved holiday tradition in the Birmingham community. The tour, which features five unique and beautifully appointed homes, includes a holiday gift market and festive seasonal fare at the Samford President's Home. Proceeds from the Christmas Home Tour provide scholarships for students with significant financial need and challenging circumstances.


text:
5484 Інода (5484 Inoda) — астероїд головного поясу, відкритий 7 листопада 1990 року.

Тіссеранів параметр щодо Юпітера — 3,472.

Примітки

Див. також
 Список астероїдів (5401-5500)

Посилання

 http://www.minorplanetcenter.net/iau/lists/NumberedMPs

Астрономічні об'єкти, відкриті 1990
Головний пояс астероїдів


text:
Q: Google search box not working, no console errors I'm practicing coding jQuery and Ajax and making a plain Google search box, but it won't work. There's no console errors and debugging in Chrome doesn't help much. Here's the code:
<!DOCTYPE html>

<meta charset="ISO-8859-1">
<title>Insert title here</title>

        <form name="input" method="get">
            Google it: <input type="text" name="googleit" />

 <input
                id="button" type="button" value="let me google that for you" />
        </form>

What's wrong with this code?

A: You can't do a cross-domain call that easily, it's restricted by Same Origin Policy. Check your network tab, it should state that the Request failed.
Also you didn't even hand over the value of your input-field. You should append it to the url like this ?q=hello.
        $.ajax({
            url : "http://www.google.com/search?q=" + $("input").val(),
            dataType : "html",

You need a so called JSONP-call to access other domains.
Take a look at the Google Search API.

redpajama_set_name: RedPajamaStackExchange


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I am an Associate Professor in the Visual Arts Department at Brock University (St. Catharines, Ontario, Canada) where I teach courses in the history of art and visual culture. I am a Faculty Affiliate in Brock's Social Justice & Equity Studies graduate program, a founding member of the Social Justice Research Institute at Brock, and a Fellow of the Oxford Centre for Animal Ethics. My current research focuses on the relationship between art and animal advocacy.
When I'm not teaching, writing, doing research, or academic administrative work you might find me volunteering at a farm sanctuary, rescuing cats, working in the garden, or cooking vegan food. I am also the co-founder of Niagara VegFest.


text:
\section{Introduction}
\label{sec:introduction}
Positronium (Ps), a bound state of an electron and a positron, is a purely leptonic system
which allows for very sensitive tests of Quantum ElectroDynamics (QED).
The precise measurement of the hyperfine splitting between orthopositronium (o-Ps, 1$^3S_1$) and parapositronium (p-Ps, 1$^1S_0$) (Ps-HFS) provides a good test of bound state QED.
Ps-HFS is expected to be relatively large (for example compared to hydrogen HFS) due to a relatively large
spin-spin interaction, and also due to the contribution from vacuum oscillation
(o-Ps $ \rightarrow \gamma ^{\ast} \rightarrow$ o-Ps).
The contribution from vacuum oscillation is sensitive to new physics beyond the Standard Model.

Figure \ref{fig:history} shows the measured and theoretical values of Ps-HFS.
The combined value from the results of the previous 2 experiments is
$\Delta _{\mathrm{HFS}} ^{\mathrm{exp}} = 203.388\,65(67)\,\mathrm{GHz} \,(3.3\,\mathrm{ppm})$
~\cite{HUGHES-V,MILLS-II}.
Recent developments in NonRelativistic QED (NRQED) have added
$\mathrm{O}(\alpha ^3 \ln \alpha)$ corrections to the theoretical prediction which now stands at
$\Delta_{\mathrm{HFS}} ^{\mathrm{th}} = 203.391\,69(41)\,\mathrm{GHz}\,(2.0\,\mathrm{ppm})$~\cite{HFS-ORDER3}.
The discrepancy of 3.04(79)\,MHz (15\,ppm, 3.9$\sigma$) between $\Delta _{\mathrm{HFS}} ^{\mathrm{exp}}$
and $\Delta_{\mathrm{HFS}} ^{\mathrm{th}}$ might either be due to the common systematic uncertainties in the previous experiments or to
new physics beyond the Standard Model.

\begin{figure}
\begin{center}
\includegraphics[width=0.4\textwidth]{hfsplot1.eps}
\caption{\label{fig:history}Measured and theoretical values of Ps-HFS.}
\end{center}
\end{figure}

There are two possible common systematic uncertainties in the previous experiments.
One is the unthermalized o-Ps contribution which results in an underestimation of the material effect.
This effect has already been shown to be significant~\cite{KATAOKA, KATAOKA-D, ASAI} in the
o-Ps lifetime puzzle.
The other is the uncertainty in the magnetic field uniformity which was cited as
the most significant systematic error by previous experimenters.

\section{Theory of Experiment}
\label{sec:theoryofexperiment}
\subsection{Measurement using Zeeman effect}
\label{sec:measurementusingzeemaneffect}

\begin{figure}
\begin{center}
\includegraphics[width=0.3\textwidth]{Pslevel.eps}
\caption{\label{fig:pslevel}Zeeman energy levels of Ps in its ground state. The arrows $\uparrow, \downarrow$ means
the spin up and down of electron, and the arrows $\Uparrow, \Downarrow$ means the spin up and down of positron.}
\end{center}
\end{figure}

The energy levels of the ground state of Ps are shown as a function of static magnetic field
in Figure \ref{fig:pslevel}. Due to technical difficulties in directly stimulating
$\Delta _{\mathrm{HFS}}$, we make an indirect measurement by stimulating the
transition $\Delta _{\mathrm{mix}}$. This is the same approach as previous experiments.
The relationship between $\Delta _{\mathrm{HFS}}$ and $\Delta _{\mathrm{mix}}$ is
approximately given by the Breit-Rabi equation
\begin{equation}
\Delta _{\mathrm{mix}} \simeq \frac{1}{2} \Delta _{\mathrm{HFS}} \left( \sqrt{1+4x^2} - 1 \right) \, ,
\label{eq:Zeeman}
\end{equation}
in which $x=g^{\prime}\mu _B B  / h\Delta _{\mathrm{HFS}}$, $g^{\prime} = g\left( 1-\frac{5}{24} \alpha ^2 \right)$
is the $g$ factor for a positron (electron) in Ps~\cite{G-FACTOR},
$\mu _B$ is the Bohr magneton, $B$ is the static magnetic field, and $h$ is the Plank constant.

In a static magnetic field, the $|S, m_z \rangle = |0,0 \rangle $,
where $S$ is the total spin of Ps and $m_z$ is
the magnetic quantum number of Ps along with z-axis (direction of static magnetic field),
state mixes with the $|1,0 \rangle$ state
hence the $|+\rangle$ state annihilates into 2 $\gamma$-rays with a lifetime of about
8\,ns (with our experimental conditions).
The $|1, \pm 1 \rangle$ states annihilate into 3 $\gamma$-rays with a lifetime of
about 140\,ns. When a microwave field with a frequency of $\Delta _{\mathrm{mix}}$ is
applied, transitions between the $|+\rangle$ state and the $|1, \pm 1 \rangle$ states are
induced so that the 2 $\gamma$-ray annihilation rate increases and the 3 $\gamma$-ray
annihilation rate decreases.
This change of annihilation rates is our experimental signal.

Our experimental resonance line shape is obtained using density matrix.
We use the basis for four spin eigenstates of Ps as $\left( \psi _0, \psi _1,
\psi _2, \psi _3 \right) \equiv \left( | 0, 0 \rangle ,
| 1, 0\rangle , | 1, 1\rangle , | 1, -1 \rangle \right) $. We apply a magnetic field
\begin{equation}
 \mbox{\boldmath $B$} (t) = B {\bf e}_{\mathrm{z}} + B_0 {\bf e}_{\mathrm{x}} \cos \left( \omega t \right)\,,
\end{equation}
where ${\bf e}_{\mathrm{z}}$, ${\bf e}_{\mathrm{x}}$ are the unit vectors for z, x direction respectively,
$B_0$ is magnetic field strength of microwaves, and $\omega$ is the frequency of microwaves.
Then the Hamiltonian $\mbox{\boldmath $H$}$ becomes
\begin{equation}
\mbox{\boldmath $H$} = \left(
\begin{array}{cccc}
-\frac{1}{2} - \frac{\mathrm{i}}{2} \gamma _{\mathrm{s}} & x & -y & y \\
x & \frac{1}{2}-\frac{\mathrm{i}}{2} \gamma _{\mathrm{t}} & 0 & 0 \\
-y & 0 & \frac{1}{2}-\frac{\mathrm{i}}{2}\gamma _{\mathrm{t}} & 0 \\
y & 0 & 0 & \frac{1}{2}-\frac{\mathrm{i}}{2}\gamma _{\mathrm{t}}
\end{array}
\right) h \Delta _{\mathrm{HFS}} \, ,
\end{equation}
where $y = C_y \frac{ g^{\prime } \mu _B B_0 }{h \Delta _{\mathrm{HFS}}} \cos \left( \omega t \right)$,
$C_y$ is a constant,
$\gamma _{\mathrm{s}} = \frac{ \Gamma _{\textrm{p-Ps}}}{2\pi \Delta _{\mathrm{HFS}}}$,
$\gamma _{\mathrm{t}} = \frac{ \Gamma _{\textrm{o-Ps}}}{2\pi \Delta _{\mathrm{HFS}}}$,
$\Gamma _{\textrm{p-Ps}}$ is the decay rate of p-Ps, and $\Gamma _{\textrm{o-Ps}}$ is that of o-Ps.
The most recent and precise experimental values are
$\Gamma _{\textrm{o-Ps}} = 7.040\,1(7)\,\mu\mathrm{s}^{-1}$~\cite{KATAOKA} and
$\Gamma _{\textrm{p-Ps}} = 7.990\,9(17)\,\mathrm{ns}^{-1}$~\cite{GAMMA-0}.

From the time-dependent Schr\"{o}dinger equation, the $4\times 4$ density matrix $\mbox{\boldmath $\rho$}(t)$ is given by
\begin{equation}
\label{eq:rho}
\mathrm{i} \hbar \dot{\mbox{\boldmath $\rho$} } = \mbox{\boldmath $H$} \mbox{\boldmath $\rho$} -
 \mbox{\boldmath $\rho$} \mbox{\boldmath $H$} ^{\dagger } \, ,
\end{equation}
where the i,j-element of $\mbox{\boldmath $\rho$}(t)$ is defined as
$\rho _{\mathrm{ij}} (t) \equiv \langle \psi _{\mathrm{i}} |
\psi (t) \rangle \langle \psi (t) | \psi _{\mathrm{j}} \rangle $.
If we take the initial state to be unpolarized, $\mbox{\boldmath $\rho$} (0) = \mathrm{diag} \left(\frac{1}{4},
\frac{1}{4}, \frac{1}{4}, \frac{1}{4} \right)$.

The 2$\gamma$-ray annihilation probability $S_{2\gamma}$ and 3$\gamma$-ray annihilation probability $S_{3\gamma}$,
between $t=t_0$ and $t=t_1$, are obtained by
\begin{equation}
\label{eq:s2gamma}
S_{2\gamma} = \Gamma _{\textrm{p-Ps} } \int _{t_0} ^{t_1} \rho _{00}(t) dt\,,
\end{equation}
\begin{equation}
\label{eq:s3gamma}
S_{3\gamma } = \Gamma _{\textrm{o-Ps} } \int _{t_0} ^{t_1}
\left( \rho _{11}(t) + \rho _{22}(t) + \rho _{33}(t) \right) dt\, .
\end{equation}

\subsection{Ps Thermalization Effect}
\label{sec:psthermalizationeffect}
Forming Ps needs material to provide electrons, but
material around Ps makes electric field and changes $\Delta _{\mathrm{HFS}}$.
This effect is called the Stark effect.
The material effect must be properly considered to evaluate $\Delta _{\mathrm{HFS}}$ in vacuum.
In the previous experiments,
the material effect on $\Delta _{\mathrm{HFS}}$ was considered to be proportional to the material (gas) density.
$\Delta _{\mathrm{HFS}}$ was measured at various gas density, and they were extrapolated linearly to zero
density~\cite{HUGHES-V, MILLS-II}.
But this extrapolation method can make large systematic error enough to account for the
discrepancy between $\Delta _{\mathrm{HFS}} ^{\mathrm{exp}}$
and $\Delta_{\mathrm{HFS}} ^{\mathrm{th}}$.

Formed Ps has the initial energy of O(eV).
Positronium loses its energy when it collides with material, and finally its energy becomes to
room temperature ($\sim1/30\,\mathrm{eV}$).
This process is called thermalization.
The material effect between $t=t_0$ and $t=t_1$ is proportional to
\begin{equation}
\label{eq:materialeffect}
 \int _{t_0} ^{t_1} f(t) \left( \rho _{00} (t) (B_0 \neq 0) - \rho _{00} (t) (B_0 = 0) \right) dt\,,
\end{equation}
where $f(t) \sim n \sigma v(t) $ is the collision rate of Ps with material,
$n$ is the number density of material, $\sigma $ is the typical cross section of collision,
and $v(t)$ is the mean velocity of Ps. In the previous experiments,
timing information was not measured so that $t_0 = 0$ and $t_1 = \infty$.
The effect is proportional to the material density if the thermalization occurs much faster than the o-Ps lifetime,
but the thermalization time scale becomes large especially at low material density, which
makes nonlinear effect on $\Delta _{\mathrm{HFS}}$.

The nonlinear effect can be estimated using the thermalization model~\cite{NETSUKA-3},
\begin{equation}
\frac{ dE_{\mathrm{av}}(t)}{dt} =
- \sqrt{2 m_{\mathrm{Ps}}E_{\mathrm{av}}(t)}\left(E_{\mathrm{av}}(t) - \frac{3}{2}k T \right)
 \frac{8}{3}\sqrt{\frac{2}{3\pi}} \frac{2\sigma _{\mathrm{m}} n}{M} \,,
\end{equation}
where $E_{\mathrm{av}}(t)$ is the average Ps energy, $m_{\mathrm{Ps}}$ is the Ps mass,
$M$ is the mass of the gas molecule, $T$ is the temperature of the gas, $k$ is the Boltzmann constant, and
$ \frac{8}{3}\sqrt{\frac{2}{3\pi}} \frac{2\sigma _{\mathrm{m}} n}{M}$ means the collision effect.
The solution of this equation is~\cite{NETSUKA-2}
\begin{equation}
\label{eq:thermalization}
E_{\mathrm{av}}(t) = \left( \frac{1+A e^{-bt}}{1-Ae^{-bt}} \right) ^2 \frac{3}{2}k T\,,
\end{equation}
where $b = \frac{8}{3}\sqrt{\frac{2}{3\pi}} \frac{2\sigma _{\mathrm{m}} n }{M} \sqrt{ 3m_{\mathrm{Ps}} k T}$,
$ A = \frac{ \sqrt{E_0} - \sqrt{ \frac{3}{2} k T }}{ \sqrt{E_0} + \sqrt{ \frac{3}{2} k T } }$,
and $E_0 \equiv E_{\mathrm{av}}(0)$ is the initial energy of Ps.

Figure \ref{fig:nonlinear} shows the best fit result of the previous experimental data from Ref.~\cite{HUGHES-V}
considering nonlinear material effect using Equations (\ref{eq:materialeffect}) and (\ref{eq:thermalization})
with parameters $E_0 = 2.07\,\mathrm{eV}$ and $\sigma _{\mathrm{m}} = 13.0$\,\AA$^2$~\cite{NETSUKA-5},
compared with linear fitting. The nonlinear effect can be clearly seen at low density, and it can
explain the discrepancy between $\Delta _{\mathrm{HFS}} ^{\mathrm{exp}}$
and $\Delta_{\mathrm{HFS}} ^{\mathrm{th}}$ (the best fit value including nonlinear effect is
$\Delta _{\mathrm{HFS}} = 203.392\,80(95)\,\mathrm{GHz}$).
But $\sigma _{\mathrm{m}} = 37 \pm 10$\,\AA$^2$ from Ref.~\cite{NETSUKA-3}, which is not consistent
with the value of Ref.~\cite{NETSUKA-5}, affects only about 5\,ppm and cannot explain the discrepancy.
Therefore, new independent measurement of Ps thermalization is needed.

\begin{figure}
\begin{center}
\includegraphics[width=0.4\textwidth]{data_fitting.eps}
\caption{\label{fig:nonlinear}(Color online) Thermalization effect on $\Delta _{\mathrm{HFS}}$.
The circles and error bars are the data of Ref.~\cite{HUGHES-V}, the solid line is the linear fit,
the dashed line is the best fit including Ps thermalization effect, and the red band is the
$\mathrm{O} (\alpha ^3 \ln \alpha )$ QED prediction in vacuum.}
\end{center}
\end{figure}

\subsection{Our new methods}
\label{sec:ournewmethods}
Our new methods will significantly reduce the systematic errors present in previous experiments;
the Ps thermalization effect and the non-uniformity of the magnetic field.
The main improvements in our experiment are the large bore superconducting magnet,
$\beta$-tagging system, and high performance $\gamma$-ray detectors.
Details are discussed in the following sections.

\section{Prototype Run}
\label{sec:prototyperun}
The prototype run of the measurement with new methods has been performed.

\subsection{Experimental Setup}
\label{sec:experimentalsetup}
A schematic diagram of the experimental setup of the prototype run
is shown in Figure~\ref{fig:schematic}.

\begin{figure}
\begin{center}
\includegraphics[width=0.48\textwidth]{Ishida_Fig3.eps}
\caption{\label{fig:schematic}Schematic diagram of the experimental setup of the prototype run (top view in magnet).}
\end{center}
\end{figure}

\subsubsection{Large bore superconducting magnet}
\label{sec:largeboresuperconductingmagnet}
A large bore superconducting magnet is
used to produce the magnetic field $B \sim 0.866\,\mathrm{T}$ which induces the Zeeman splitting.
The bore diameter of the magnet is 800\,mm, and its length is 2\,m.
The large bore diameter means that there is good uniformity in the magnetic field in the
region where Ps is formed.
Furthermore, the magnet is operated in persistent current mode, making the stability of the magnetic field
better than $\pm$1\,ppm.

The magnetic field distribution was measured using a proton NMR magnetometer (ECHO Electronics EFM-150HM-AX)
with a clock synthesizer (NF Corporation CK1615 PA-001-0312). Calibration uncertainty of the system is
less than 1\,ppm. Non-uniformity of the magnetic field in a whole volume of RF cavity is
23.1\,ppm (RMS) without any compensation coils. The non-uniformity decreases to 10.4\,ppm when weighted by
RF power and positron stop position distribution.

\subsubsection{$\beta$-tagging system and timing information}
\label{sec:betataggingsystemandtiminginformation}
The positron source is 19\,$\mu$Ci (700\,kBq) of $ \mathrm{^{22}Na}$ (Eckert \& Ziegler POSN-22).
A plastic scintillator (NE102A) 10\,mm in diameter and 0.2\,mm thick is used to tag positrons emitted from the $\mathrm{^{22}Na}$.
The scintillation light is detected by fine mesh photomultiplier tubes (PMT: HAMAMATSU H6614-70MOD)
and provides a start signal which corresponds to the time of Ps formation.
The timing resolution is 1.0\,ns (1$\sigma$).
The positron then enters the microwave cavity, forming Ps in the gas contained therein.

Ps decays into photons that are detected with LaBr$_3$\,(Ce) scintillators (Saint-Gobain BrilLanCe$^{\mathrm{TM}}$ 380).
Accumulating measurements of the times of positron emission and $\gamma$-detection results in
decay curves of Ps as shown in Figure \ref{fig:timing_spectra}.
The timing information is used to improve the accuracy of the measurement of $\Delta _{\mathrm{HFS}}$ as follows:
\begin{enumerate}
\item Imposing a time cut means that we can select well thermalized Ps, reducing the unthermalized o-Ps contribution.
It should also be possible to precisely measure the contributions of
unthermalized o-Ps, and of material effects (we plan to make such measurements in future runs).
\item A time cut also allows us to avoid the prompt peak (contributions of
simple annihilation and of fast p-Ps decay), which greatly increases the S/N of the measurement (by about a factor of 20).
\end{enumerate}

\subsubsection{High performance $\gamma$-ray detectors}
\label{sec:highperformancegammaraydetectors}
Six $\gamma$-ray detectors are located around the microwave cavity to detect
the 511\,keV annihilation $\gamma$-rays.
LaBr$_3$ scintillators, 1.5 inches in diameter and 2 inches long are used.
The scintillation light is detected by fine mesh PMT through the UVT light guide.
Without light guide, LaBr$_3$ scintillators have
good energy resolution (4\% FWHM at 511\,keV) and timing resolution (0.2\,ns FWHM at 511\,keV),
and have a short decay constant (16\,ns).
The good energy resolution and the high counting rate of LaBr$_3$ results in very good overall performance
for measuring Zeeman transitions.
In particular the good energy resolution allows us to efficiently separate 2$\gamma$ events from
3$\gamma$ events, negating the need to use a back-to-back geometry to select 2$\gamma$ events, thus
greatly increasing the acceptance of our setup.

This $\gamma$-ray detector system greatly reduces the statistical error in the measurement.

\subsubsection{RF system}
\label{sec:rfsystem}
Microwaves are produced by
a local oscillator signal generator (ROHDE \& SCHWARZ SMV 03) and amplified to 500\,W with a
GaN amplifier (R\&K A2856BW200-5057-R).

The microwave cavity is made with oxygen-free copper;
the inside of the cavity is a cylinder 128\,mm in diameter and
100\,mm long. The side wall of the cavity is only 2\,mm thick in order to
allow the $\gamma$-rays to efficiently escape.
The cavity is operated in the TM$_{110}$ mode. The resonant frequency is 2.856\,6\,GHz and
$Q_L = 14,700 \pm 50$. The cavity is filled with gas
(90\% N$_2$ and 10\% iso-C$_4$H$_{10}$) with a gas-handling system. Iso-C$_4$H$_{10}$ is used as the quenching gas
to remove background 2 $\gamma$-ray annihilation.

\subsubsection{Monte Calro simulation}
\label{sec:montecalrosimulation}
The Monte Calro simulation to use in analysis is performed using Geant4~\cite{GEANT4}.
The low energy physics package PENELOPE~\cite{PENELOPE} is used and the geometry of the experimental setup is
carefully input.
The simulation is produced at each magnetic field strength and gas density.

\subsubsection{Data acquisition}
\label{sec:dataacquisition}
The prototype run was performed from 2 July 2009 to 24 September 2009
using the large bore magnet with no compensation (compensation magnets to reduce
the uniformity to O(ppm) are planned but are not yet installed).
In the overall period, the trigger rate was about 3.6\,kHz and the data acquisition rate was about
650\,Hz. The data acquisition was performed using NIM and CAMAC system.

The trigger signal is the coincidence signal of $\beta$-tagging system and $\gamma$-ray detectors.
Timing information of all PMT are obtained with a 2\,GHz direct clock counting Time-to-Digital Converter
(TDC: GNC-060)~\cite{KATAOKA, KATAOKA-D}.
A charge ADC (CAEN C1205) is used to measure the energy information of the LaBr$_3$ crystals while
another charge ADC is used to measure the energy information of the plastic scintillators.
A crate controller (TOYO CC/NET) is used and obtained data are stored in a HDD of a Linux PC via Ethernet.
The Zeeman transition has been measured at various magnetic field strengths with a fixed RF frequency and power.
The transition resonance lines are obtained at two gas densities (1.350\,1\,amagat and 0.891\,6\,amagat).

\subsection{Analysis}
\label{sec:analysis}

\subsubsection{Data analysis}
\label{sec:dataanalysis}

\begin{figure}
\begin{center}
\includegraphics[width=0.4\textwidth]{timing_window.eps}
\caption{\label{fig:timing_spectra}(Color online) Decay curves of Ps. The red line is on-resonance (0.865\,816\,9\,T) RF\,ON, and the black line is RF\,OFF.
The timing window of 35--155\,ns is also indicated. The decay rate of Ps increases with RF because of the Zeeman transition.}
\end{center}
\end{figure}

\begin{figure}
\begin{center}
\subfigure[Typical fitting of energy spectrum (RF-OFF).
The black points are the data, the red line is $S_{2\gamma} ^{\mathrm{MC}}$, the blue line is $S_{3\gamma } ^{\mathrm{MC}}$,
and the pink line is sum of the Monte Calro spectra.]{
	\includegraphics[width=0.4\textwidth]{typical_fit_with_mc.eps}
	\label{fig:energy_spectraa}}
\subfigure[Typical fitting of energy spectrum (RF-ON).
The black points are the data, the red line is $S_{2\gamma ,\mathrm{in}} ^{\mathrm{MC}}$,
the blue line is $S_{3\gamma ,\mathrm{in}} ^{\mathrm{MC}}$,
the green line is $S_{2\gamma ,\mathrm{out}} ^{\mathrm{MC}}$,
the aqua line is $S_{3\gamma ,\mathrm{out}} ^{\mathrm{MC}}$,
and the pink line is sum of the Monte Calro spectra. $A_{\mathrm{OFF}}$ and $\beta $ are
fixed with the fitted values of RF-OFF, so that the free parameters are $A_{\mathrm{ON}}$ and $\Gamma $.]{
	\includegraphics[width=0.4\textwidth]{typical_fit_with_mc_on.eps}
	\label{fig:energy_spectrab}}
	\caption{(Color online) Typical energy spectra and its fitting with Monte Calro simulation.
The data at 1.350\,1\,amagat, 0.865\,816\,9\,T are shown and the spectra are normalized by the live time.}
	\label{fig:energy_spectra}
\end{center}
\end{figure}

Figure \ref{fig:timing_spectra} shows examples of measured timing spectra. The prompt peak coming from annihilation and
$|-\rangle$ decay is followed by the decay curve of $|+\rangle$ and $m_z=\pm 1$ states, then the constant accidental spectrum.
A timing window of 35--155 ns is applied to select transition events.
Figure \ref{fig:energy_spectra} shows energy spectra, which are obtained by
subtracting the accidental contribution using the timing window $t = $700--850\,ns.

The energy spectra are fitted using Monte Calro simulation.
The energy spectrum of RF-OFF $S_{\mathrm{OFF}}$ can be expressed as
\begin{equation}
S_{\mathrm{OFF}} = A_{\mathrm{OFF}} \left( S_{\mathrm{3\gamma}} ^{\mathrm{MC}} +
\beta  S_{\mathrm{2\gamma}} ^{\mathrm{MC}} \right) \, ,
\end{equation}
where $A_{\mathrm{OFF}}$ is a normalizing constant, $\beta $ is a $2\gamma / 3\gamma $ decay ratio of RF-OFF,
$S_{\mathrm{2\gamma}} ^{\mathrm{MC}}$ is a Monte Calro simulated energy spectrum of $2\gamma $ decay,
and $S_{\mathrm{3\gamma }} ^{\mathrm{MC}} $ is that of $3\gamma $ decay.
On the other hand, the energy specrum of RF-ON $S_{\mathrm{ON}}$ can be expressed as
\begin{equation}
S_{\mathrm{ON}} = A_{\mathrm{ON}} \left( S_{\mathrm{3\gamma}, \mathrm{in}} ^{\mathrm{MC}} +
\Gamma  S_{\mathrm{2\gamma}, \mathrm{in}} ^{\mathrm{MC}} \right) +
A_{\mathrm{OFF}} \left( S_{\mathrm{3\gamma}, \mathrm{out}} ^{\mathrm{MC}} +
\beta  S_{\mathrm{2\gamma}, \mathrm{out}} ^{\mathrm{MC}} \right) \, ,
\end{equation}
where $A_{\mathrm{ON}}$ is a normalizing constant and $\Gamma $ is a $2\gamma / 3\gamma $ decay ratio of RF-ON.
The subscript ``in" and ``out" means the spectrum of $\gamma$-rays from Ps decays in the volume where RF power is applied
or not applied, respectively.

Typical fitted results are also shown in Figure \ref{fig:energy_spectra}. Figure \ref{fig:energy_spectraa} is RF-OFF,
and \ref{fig:energy_spectrab} is RF-ON.
The energy spectrum is measured at different magnetic field strengths.
The fitting range is 370--545\,keV.
All the spectra are fitted successfully using MINUIT~\cite{MINUIT}.

\begin{figure}
\begin{center}
\includegraphics[width=0.4\textwidth]{resonance_line_13501.eps}
\caption{\label{fig:resonance_line}Resonance line at 1.350\,1 amagat gas density. The circles and error bars are the data, and
the solid line is the best fit result.
The error bars include errors from statistics of data, statistics of Monte Calro simulation, uncertainty of RF power, and uncertainty of
$Q_L$ value of the RF cavity.}
\end{center}
\end{figure}

We take $\Gamma - \beta $ as an amount of Zeeman transition.
An example of resonance line obtained is shown in Figure \ref{fig:resonance_line}.
Resonance lines can be fitted by
$S_{2\gamma }/S_{3\gamma } (\textrm{RF-ON}) - S_{2\gamma }/S_{3\gamma } (\textrm{RF-OFF})$ .
The theoretical function is calculated from Equations (\ref{eq:s2gamma}) and (\ref{eq:s3gamma}) numerically
using RKF45 formula, with contributions from pick-off and slow positron.
The typical $B_0$ is 14.2\,G. The RF-OFF function is obtained by substitute 0 for $B_0$.
Then the free parameters of fitting are $\Delta _{\mathrm{HFS}}$ and $C_y$.
The fitting results are summarized in Table~\ref{tab:fittingresult}.
We use $-33\,\mathrm{ppm/amagat}$~\cite{HUGHES-V} as the material effect and
obtain $\Delta _{\mathrm{HFS}}$ in vacuum.

\begin{center}
\begin{table}
\caption{\label{tab:fittingresult}Fitting result of the resonance lines. These uncertainties include
errors from statistics of data, statistics of Monte Calro simulation, uncertainty of RF power, and uncertainty of
$Q_L$ value of the RF cavity.}
\begin{center}
\begin{tabular}{crrr}
\hline \hline
Gas density & $\Delta _{\mathrm{HFS}}$ & Relative error & $\chi ^2 / \mathrm{ndf}$ \\
(amagat) & (GHz) & (ppm) & \\
\hline
1.350\,1(71) & 203.368\,3(55) & 27 & 0.910 \\
0.891\,6(23) & 203.379\,3(70) & 34 & 0.483 \\
\hline \hline
\end{tabular}
\end{center}
\end{table}
\end{center}

\subsubsection{Systematic Errors}
\label{sec:systematicerrors}
Systematic errors of the prototype run are summarized in Table~\ref{tab:systematicerror}.
\begin{enumerate}
\item {\it Magnetic Field}. The largest uncertainty in the prototype run is non-uniformity of the
magnetic field. The weighted non-uniformity is 10.4\,ppm.
The offset and reproducibility of the magnetic field is measured to be 2\,ppm.
The calibration uncertainty of NMR magnetometer is 1\,ppm.
These uncertainties are doubled because
$\Delta _{\mathrm{HFS}}$ is approximately proportional to square of the magnetic field strength.
\item {\it Monte Calro Simulation}. The magnetic field dependence of $\beta$ is not
exactly reproduced by the energy spectra fitting with Monte Calro simulation.
From the difference between theoretical dependence and fitted result, this effect is
estimated to be 18\,ppm. The statistical uncertainty of Monte Calro simulation is 17\,ppm.
\item {\it RF System}. The uncertainty of $Q_L$ value of RF cavity comes from
reproducibility of the RF environment ($\sim 5\%$) and
uncertainty of the $Q_L$ measurement method (0.6\%). Its effect on $\Delta _{\mathrm{HFS}}$ is
estimated to be 6\,ppm.
RF power uncertainty comes from reproducibility of the RF environment ($\sim 2\%$),
uncertainty of power meters (0.05\%), and uncertainty of the power meter calibration of
temperature dependence (0.03\%/K). It contributes to the error on $\Delta _{\mathrm{HFS}}$ by
5\,ppm.
The uncertainty of RF frequency is 5\,ppm. It directly affects $\Delta _{\mathrm{HFS}}$ because
$\Delta _{\mathrm{HFS}}$ is approximately proportional to inverse of RF frequency.
\item {\it Material Effect}. Thermalization of Ps can affect $\Delta _{\mathrm{HFS}}$ by up to 20\,ppm, but
it has been not yet measured. Gas density dependence has not been measured in the prototype run, so
we have used the value from previous experiment. The uncertainty of the density dependence is
4\,ppm/amagat~\cite{HUGHES-V}, and the uncertainty from iso-C$_{4}$H$_{10}$ is estimated to be less than 7.7\,ppm/amagat.
These result in 7\,ppm uncertainty of $\Delta_{\mathrm{HFS}}$.
\end{enumerate}
Other uncertainties are considered to be negligible. The systematic errors discussed above are summed in quadrature.

\begin{center}
\begin{table}
\caption{\label{tab:systematicerror}Summary of Systematic errors of the prototype run.}
\begin{center}
\begin{tabular}{lr}
\hline \hline
Source & Errors in $\Delta _{\mathrm{HFS}}$ (ppm) \\
\hline
{\it Magnetic Field:} & \\
~~Non-uniformity & 21 \\
~~Offset and reproducibility & 4 \\
~~NMR measurement & 2 \\
{\it Monte Calro Simulation:} & \\
~~Magnetic field dependence & 18 \\
~~Statistics & 17 \\
{\it RF System:} & \\
~~$Q_L$ value of RF cavity & 6 \\
~~RF power & 5 \\
~~RF frequency & 5 \\
{\it Material Effect:} & \\
~~Thermalization of Ps & $<20$ \\
~~Gas density dependence & 7 \\
\hline
Quadrature sum & 40 \\
\hline \hline
\end{tabular}
\end{center}
\end{table}
\end{center}

\subsection{Result}
\label{sec:result}

The value of $\Delta_{\mathrm{HFS}}$ obtained from the prototype run is
\begin{eqnarray}
\Delta _{\mathrm{HFS}} &=& 203.380\,4 \pm 0.002\,2 (\mathrm{stat.}, 11\,\mathrm{ppm}) \nonumber \\
& & \pm 0.008\,1 (\mathrm{sys.},40\,\mathrm{ppm})
\, \mathrm{GHz}\, ,
\end{eqnarray}
which is consistent with both of the previous experimental values and with the theoretical value.
The uncertainty is an order of magnitude larger than the goal precision of O(ppm).

\subsection{Next steps}
The following improvements are planned for future measurements:
\begin{enumerate}
\item Compensation magnets will be installed and O(ppm) magnetic field uniformity is
expected to be achieved.
\item The Monte Calro simulation will be studied to reproduce the magnetic field dependence of
energy spectra of Ps decays. Statistics of simulation will be reduced to O(ppm).
\item The errors from RF system will be reduced to O(ppm) by carefully controlling the
environment (especially the temperature) of the experiment.
\item Measurements at various pressures of gas will be performed to estimate
the material effect (the Stark effect). The accumulation of these measurements will
result in an O(ppm) statistical error within a few years.
\item The timing information allows for a measurement of Ps thermalization as a function of
time~\cite{KATAOKA, KATAOKA-D, ASAI}. We can thus precisely measure the material effect including the
thermalization effect.
\end{enumerate}

\section{Conclusion}
\label{sec:conclusion}
A new experiment to measure the Ps-HFS which reduces possible common uncertainties in previous experiments
has been constructed and the prototype run has been finished. A value of
$\Delta _{\mathrm{HFS}} = 203.380\,4 \pm 0.002\,2 (\mathrm{stat.}) \pm 0.008\,1 (\mathrm{sys.}) \, \mathrm{GHz} \, (41\,\mathrm{ppm})$ has been obtained, which is
consistent with both of the previous experimental values and with the theoretical calculation. Development of compensation magnets
is underway with a view to obtaining O(ppm) magnetic field homogeneity for the final run.
The final run will start soon.
A new result with an accuracy of O(ppm) will be
obtained within a few years which will be an independent check of the discrepancy between the present experimental values and the QED prediction.

\bibliographystyle{elsarticle-num}

redpajama_set_name: RedPajamaArXiv


text:
Gründerzeit (grundlæggertiden) betegnes normalt den periode i tysk historie, der strækker sig fra tiden umiddelbart efter den tyske sejr i den tysk-franske krig 1870/1871 frem til århundredeskiftet. Iblandt hører man den også brugt om den tilsvarende periode i østrigsk historie.

I denne periode blev der bygget flittigt over alt i det tyske kejserrige, og den specielle arkitektur man byggede i kaldes derfor "Gründerzeit"-stil. Bygningerne var især finere beboelsesejendomme, som de f.eks. fra Østerbro i København, men mange offentlige tyske bygninger bygget i denne periode er også bygget i denne stil. Mest prominente eksempel er nok Rigsdagsbygningen i Berlin. Man taler om, at byggestilen var præget af den tids prægende idehistoriske tankegang, historisme, hvor man greb tilbage til ikke bare ældre klassiske stilarter, men også benyttede sig af nationalromantiske forestillinger om Middelalderen.

I den tyske litteratur har den samtidige forfatter Wilhelm Raabe beskrevet perioden i et kritisk lys.

Årsager til Gründerzeit

Det tyske kejserrige var på dette tidspunkt inde i en rivende udvikling. Industrialiseringen slog sent igennem i Tyskland, først i anden halvdel af det 19. århundrede, men da den først kom, væltede den nærmest samfundet på hovedet fra den ene dag til den anden. I løbet af få år var hele det tyske område spækket med jernbaner og fabrikker. Den enorme vandring fra land til by krævede selvsagt enorme byudvidelser.

Især takket være den enorme krigsbod fra Frankrig (fem milliarder guldfranc) kunne man sætte gang i et sandt byggeboom. De mange penge fra Frankrig betød et stort økonomisk opsving for Tyskland.

Østrig i 1800-tallet
Tyskland i 1800-tallet
Stilperioder


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Q: Apache server : Reverse proxy and websockets via mod_proxy_wstunnel I have a little problem with the web sockets and my reverse proxy apache, i have upgraded in latest release 2.4.5 and loaded the module mod_proxy_wstunnel.
The httpd.conf :
     <VirtualHost *:80>
ServerAdmin webmaster@localhost
ServerName www.toto.fr
ServerAlias toto.fr

    ProxyPass /my_app  http://1X.X.X.1:8080/my_app
    ProxyPassReverse /web_pmr  http://1X.X.X.1:8080/my_app
    ProxyPassReverseCookiePath /my_app /
    ProxyPassReverseCookieDomain localhost my_app
    ProxyRequests off
    ProxyTimeout 15

        #WEBSOCKETS

        ProxyPass /my_app/BasicWebsocketServlet ws://1X.X.X.1:8080/my_app/BasicWebsocketServlet retry=0
    ProxyPassReverse /my_app/BasicWebsocketServlet ws://1X.X.X.1:8080/web_pmr/BasicWebsocketServlet retry=0

ErrorLog "logs/my_app_error.log"
LogLevel debug
CustomLog "logs/my_app_access.log" combined

<Proxy *>
              Order deny,allow
              Allow from all
</Proxy>
</VirtualHost>

When i test in my local url, websockets are working but with the reverse proxy apache no trace in tomcat logs.
List of loaded modules :
Loaded Modules: core_module (static) so_module (static) http_module (static) mpm_event_module (static) authn_file_module (shared) authn_core_module (shared) authz_host_module (shared) authz_groupfile_module (shared) authz_user_module (shared) authz_core_module (shared) access_compat_module (shared) auth_basic_module (shared) filter_module (shared) mime_module (shared) log_config_module (shared) env_module (shared) headers_module (shared) setenvif_module (shared) version_module (shared) proxy_module (shared) proxy_connect_module (shared) proxy_ftp_module (shared) proxy_http_module (shared) proxy_fcgi_module (shared) proxy_scgi_module (shared) proxy_fdpass_module (shared) proxy_wstunnel_module (shared) proxy_ajp_module (shared) proxy_balancer_module (shared) proxy_express_module (shared) slotmem_shm_module (shared) slotmem_plain_module (shared) ssl_module (shared) lbmethod_byrequests_module (shared) lbmethod_bytraffic_module (shared) lbmethod_bybusyness_module (shared) lbmethod_heartbeat_module (shared) unixd_module (shared) status_module (shared) autoindex_module (shared) dir_module (shared) alias_module (shared) rewrite_module (shared)

Thank you.

A: Trailing slash must be added to path, it's necessary to handle web socket requests as GET requests (httpd.apache.org/docs/2.4/mod/mod_proxy.html#proxypass)
something like:
ProxyPass        /my_app/BasicWebsocketServlet/ ws://1X.X.X.1:8080/my_app/BasicWebsocketServlet/ retry=0
ProxyPassReverse /my_app/BasicWebsocketServlet/ ws://1X.X.X.1:8080/web_pmr/BasicWebsocketServlet/ retry=0


There was little snowfall this winter. When there isn't a snowpack to melt in the spring, there is drought because the melting snow fills the rivers and creeks and creates spring flowers. So I thought this spring would be sad. It would be sad just like this election had been sad, the healthcare system in this country is sad, the state of the mental health of this nation is sad and so on and so forth. It would be one more thing.
But no one can predict the weather. It rained and rained at the start of this spring and the miraculous happened: flowers bloomed in a frenzy (it's been a month and I've got the same tulips blooming still), trees let out baby leaves before I could blink and the grass roared to green life.
It is one of the greenest springs I have ever known. And now that it's been going strong for a month, things are happening. The rain has not stopped and now blooming bushes are pulling down fences, sidewalks are disappearing under green and mud, lawns are growing faster than people can mow and the birds never stop singing.
During a walk, I passed by a young tree packed with chickadees. My husband thought the chickadees were cute (they were). I told him they were vying for territory, their cheeps filling the air with lust for power, trees, and land. And as I said these words, I thought of the few things we know about the Celtic pagan past and that this time of year was not a just sweet time but a pulsating, racing, hungry time. Nobody was full of food yet, that wouldn't be until later on in the summer. The sun was coming back and people obsessively followed, traced, and urged along her every movement.
This is a season when the continuation of life hangs in the balance. Will the sun come back? Will the green come back? Will the birds come back? Will we survive into the next season? Will there be plenty or starvation ahead?
I sit down to eat breakfast and look out the window. In the garden, bleeding heart flowers cascade from slender green stems. Birds disappear in the riotous lawn only to reappear again as they wing upward and away. The maples unfurl their leaves in the sun while the red oaks are more steady, slow, and cautious. A faint, tender green line the tips of their branches. A small squirrel inches to the end of a slender tree branch and places maple tree helicopter seeds in her tiny cheeks.
The holidays have taken a back seat to the sky.
I peer up at the sky every chance I get, noting clouds, colors, and motions. The leaves lie forgotten in the ditches and without their leafy apparel, the tree branches spread overhead like crones' fingers in the sky. I see through the fingers.
Summer is a claustrophobic time and winter is the great opening. We're all exposed now, to the sun and wind and elements. Gracious green canopies no longer spread out in umbrella formations, bestowing dappled light and easier breathing. No, it's time for sullen scolding winds and scudding clouds.
I position my fingers on the trunks of trees to hang on while I view skyward, nearly whisked away by the drama overhead. The great burr oaks are the best for holding. They have seen centuries and still chose to linger on in this world. They're rooted vast and deep. While I hold onto one, burr oak reminds me that time is like a spool of thread and the spool can be wound or unwound. Time backward or forward. The clouds overhead whisk by on wings of dark intent and their colors etch into my eyes and race to the brain. We are grey together, sometimes closer to white, other times to blue.
The spool unwinds and I am younger and back on my parents' farm and the clouds are racing there too and I am turning away from them while standing at window. I turn my head and my body follows and I crawl into bed under the quilt/or turn up Winter by Vivaldi/or listen to Tess Wiley's electric guitar solo/or write stories about an insane family I invented but might as well be my own.
The spool winds and I am back in my town and I am back with the oak. There are no birds flying, the wind is too strong for that, but there are squirrels in the trees, chomping fiercely and their backs and tails are as grey as the sky.


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Q: How to overflow background Image off screen Right now I'm coding a site where all of the content is positioned in the center of the page. I want a little plane icon to be positioned with its trail running off the right side of the screen.
However, the image keeps creating a horizontal scroll bar for the rest of the image.
How do i place an image where the remaining part of the image is only visible upon resizing the browser.
See attached code:
.home-planepath {
    position:absolute;
    left:50%;
    width:100%;
    height:62px;
    z-index: 1;
    margin-top:442px;
    margin-left: -440px;
    overflow: hidden;
    background:url(images/home-planepath.png) no-repeat;
}

A: You should set overflow:hidden on your container, i.e .homehover instead of .home-planepath