If a nice-looking plant could attract scads of birds, make a great mess of greens, treat cancer, AIDS, herpes, bad breath and more, and revolutionize the solar energy industry on the side, wouldn't you want it in your backyard? All of these claims and more have been made for the American Pokeweed (Phytolacca americana), an imposing perennial common in disturbed, fallow and edge areas, routinely growing taller than 6-8 feet, with large, oblong leaves and reddish stems at maturity. It's also known as poke root, poke salad (or poke sallet), poke berry, poke, inkberry, cancer root, American nightshade, pigeon berry and other names. The starring feature of Pokeweed is the flower cluster, which can host flowers, immature green berries and mature, shiny red berries all on the same clump, and there are many clumps per plant, flowering from May on into the fall. It dies back to its very large taproot each winter and re-emerges each spring. It is very insistent about that. With all this going for it, what's not to like? Well, for one thing, it's poisonous. For another, it's persistent and somewhat aggressive and difficult to eradicate. Pokeweed has its passionate defenders, implacable enemies, and some in between, who might wish it wasn't there, but have no qualms about using it for its good qualities. We have several healthy specimens in our yard, mostly around the edges in the fence or up against the house, and we appreciate it because birds find it irresistible. We never planted it. It showed up on its own, probably from the hard little seeds passing through a bird and being deposited with a handy little packet of fertilizer. It seems to generate a couple more plants each year, and we will soon have to control its spread. We pull it or chop it in places where we don't want it, but this might be only semi-effective, since it will try to come back from the root each spring. There are chemical treatments, if you're really desperate, including glyphosate. At least one online gardeners' forum has had a lively debate on the merits of this plant in gardens and its control. Pokeweed is one of the signature edible native plants of America, with a strong role in Native-American, African-American and Southern cultures and cuisines. The key is caution. Young leaves and stems in the spring, before any red has crept into them, are harvested by legions of foragers and boiled in at least two changes of water, discarding the water afterwards. Some, in Southern style, saute the greens with bacon drippings and crumbles, alone or mixed with other wild greens. Some also cook the young stems like asparagus, to which their flavor is compared, or cut them into rounds, like okra, coating them with cornmeal and frying them. Some just saute them in butter, with salt and pepper. They are sometimes used in making pickles. Just remember to blanch them in water first! Twice! Never eat the roots! Never. Too bad, too, because they're big and juicy. The toxins in Pokeweed, depending on what source you're working from, range from deadly to mild. They are usually concentrated in the roots, berries and seeds and include an alkaloid (phytolaccine), a resin (phytolaccatoxin), and a saponin (phytolaccigenin). Their effects can range from embarrassing to very nasty, including diarrhea, vomiting, internal bleeding, rapid heartbeat, convulsions, and much more, up to and including death. Blanching in changes of water eliminates most of the toxins from young leaves and stems, but caution is called for. Also, since the berries are a very tempting looking bright red, you might want to think twice about having this plant in places frequented by young children, because I remember what I was like as a kid. Aside from its decorative and culinary qualities , Pokeweed is useful for establishing quail habitat, since quail love the berries (birds are not affected by the toxins), and it also forms a nice shady refuge for them. It is good for attracting pollinating insects to gardens. It has been used for inks and dyes (here's how you can make your own!), making a beautiful red color, and is being studied for potential treatments for cancer and various viral diseases, among other ailments. Some folks still swear by eating a small number of berries to prevent arthritis, but you didn't hear that from me. Keep in mind that online sources of medical information often urge strong caution in using Pokeweed medicinally, or simply say "Don't do it." It has even inspired a song or two along the way. Who could forget Poke Salad Annie? One of its newest uses is in the field of solar energy generation. It seems a red dye made from the mature berries can be used to coat fiber-based solar cells, increasing their efficiency in converting sunlight into electricity. Did you know it?
If a nice-looking plant could attract scads of birds, make a great mess of greens, treat cancer, AIDS, herpes, bad breath and more, and revolutionize the solar energy industry on the side, wouldn't you want it in your backyard?
All of these claims and more have been made for the American Pokeweed (Phytolacca americana), an imposing perennial common in disturbed, fallow and edge areas, routinely growing taller than 6-8 feet, with large, oblong leaves and reddish stems at maturity. It's also known as poke root, poke salad (or poke sallet), poke berry, poke, inkberry, cancer root, American nightshade, pigeon berry and other names. The starring feature of Pokeweed is the flower cluster, which can host flowers, immature green berries and mature, shiny red berries all on the same clump, and there are many clumps per plant, flowering from May on into the fall. It dies back to its very large taproot each winter and re-emerges each spring. It is very insistent about that.
With all this going for it, what's not to like? Well, for one thing, it's poisonous. For another, it's persistent and somewhat aggressive and difficult to eradicate. Pokeweed has its passionate defenders, implacable enemies, and some in between, who might wish it wasn't there, but have no qualms about using it for its good qualities. We have several healthy specimens in our yard, mostly around the edges in the fence or up against the house, and we appreciate it because birds find it irresistible. We never planted it. It showed up on its own, probably from the hard little seeds passing through a bird and being deposited with a handy little packet of fertilizer. It seems to generate a couple more plants each year, and we will soon have to control its spread. We pull it or chop it in places where we don't want it, but this might be only semi-effective, since it will try to come back from the root each spring. There are chemical treatments, if you're really desperate, including glyphosate. At least one online gardeners' forum has had a lively debate on the merits of this plant in gardens and its control.
Pokeweed is one of the signature edible native plants of America, with a strong role in Native-American, African-American and Southern cultures and cuisines. The key is caution. Young leaves and stems in the spring, before any red has crept into them, are harvested by legions of foragers and boiled in at least two changes of water, discarding the water afterwards. Some, in Southern style, saute the greens with bacon drippings and crumbles, alone or mixed with other wild greens. Some also cook the young stems like asparagus, to which their flavor is compared, or cut them into rounds, like okra, coating them with cornmeal and frying them. Some just saute them in butter, with salt and pepper. They are sometimes used in making pickles. Just remember to blanch them in water first! Twice!
Never eat the roots! Never. Too bad, too, because they're big and juicy.
The toxins in Pokeweed, depending on what source you're working from, range from deadly to mild. They are usually concentrated in the roots, berries and seeds and include an alkaloid (phytolaccine), a resin (phytolaccatoxin), and a saponin (phytolaccigenin). Their effects can range from embarrassing to very nasty, including diarrhea, vomiting, internal bleeding, rapid heartbeat, convulsions, and much more, up to and including death. Blanching in changes of water eliminates most of the toxins from young leaves and stems, but caution is called for. Also, since the berries are a very tempting looking bright red, you might want to think twice about having this plant in places frequented by young children, because I remember what I was like as a kid.
Aside from its decorative and culinary qualities , Pokeweed is useful for establishing quail habitat, since quail love the berries (birds are not affected by the toxins), and it also forms a nice shady refuge for them. It is good for attracting pollinating insects to gardens.
It has even inspired a song or two along the way. Who could forget Poke Salad Annie?
One of its newest uses is in the field of solar energy generation. It seems a red dye made from the mature berries can be used to coat fiber-based solar cells, increasing their efficiency in converting sunlight into electricity.


text:
Over Half a Million Facebook Users Sign Up to Raid Area 51
South Africa's Jacob Zuma says corruption allegations are 'a conspiracy'
78 dead in Nepal as floods cause havoc across Asia
Man faces second sentence in Charlottesville car attack
Antofagasta plc Reko Diq project Arbitration Award
Founder of African American museum found dead in auto trunk
Hong Kong police fight with protesters
Bianca Devins murder images flood Instagram
S-400 deliveries to Turkey cause no concern in Damascus, says ambassador
Meghan McCain Blasts Republicans' "Cowardly" Silence on Trump Tweets: "It's Deeply Racist"
Northern Districts' batsmen create world record, smashing 43 runs off an over Poor Ludick's figures went from a respectable 1/42 from nine overs to a messy 1/85 from 10. Carter finished unbeaten on 102 off 77 balls while Hampton was dismissed for 95 off 66.
Harvick earns his shot at NASCAR Cup title with win at Texas After the first of the late restarts, Harvick was on the inside and was able to keep Blaney from clearing him on the backstretch. We could have won every race here. "So, thank you guys!" "The expectations are to win", Harvick told reporters.
Manu Tuilagi England return settles down squad says Ben Youngs 'I was gutted when he pulled out, but it was a tiny niggle. "We won't risk him, he's either 100 per cent fit or he's not". I'm really pleased he's able to get back out there.
Kim Davis loses Kentucky clerk re-election bid Davis was a Democrat before switching her party affiliation shortly after she refused to issue same-sex marriage licenses. Caudill addressed Davis' actions on his own campaign website and vowed to "serve every citizen of this county equally".
Le'Veon Bell hasn't talked to Steelers, unlikely to report this week Bell would surrender the final $6.84 million of his salary if he elects not to sign the franchise tender. Fitness club in North Pittsburgh on Tuesday night, a manager with L.A.
Driver charged in toddler deaths in crosswalk kills herself Horrifying video captured at the scene shows the white auto rolling into the crosswalk as the unsuspecting pedestrians are struck. She won for best featured actress in a musical in 2015 and had been due to play the same role in London's West End this summer.
Scott Boras: Why a $300 million Bryce Harper offer wasn't close But no position player has ever earned an average annual value of more than $27.5 million (Alex Rodriguez and Yoenis Cespedes). It will cost them roughly $US13 million. "I'm comfortable with the alternative (to Harper returning)", Rizzo said.
FDA approves highly effective new opioid regardless of ongoing epidemic The approval comes just a bit more than a year after President Donald Trump declared the opioid crisis a public health emergency. Experts worry that supplies of the drug will somehow make their way from doctors' offices and pharmacies to addicts.
Rohit Sharma overtakes Virat Kohli; becomes India`s leading run scorer in T20Is Rohit hit seven sixes and eight fours to post his fourth T20 century , the most by any batsman in the format at global level. India lead the three-match series 1-0. "I was reading the pitch when we were batting", he said.
Passengers delay flight over pungent planeload of durian The cause of the bad stench was a huge supply of durian fruit which was travelling in the cargo hold on the Indonesian flight. The flight eventually took off around 11:40am local time (04:40 GMT), an hour later than scheduled.
Pink Wave: Women to Flood Congress After Historic Election Night Speaking at a victory part in Washington , Democratic House Leader Nancy Pelosi said: "Tomorrow will be a new day in America". Veronica Escobar and Sylvia Garcia won House races in Texas, making them the first Latina women to ever represent the state.
Rihanna Reportedly Serves Notice After Her Song Is Used At Trump Rally According to Rolling Stone , Rihanna's legal representatives have sent a cease and desist letter to Trump's White House counsel. He wrote that these licenses "were not intended for such craven political purposes, without the songwriters' consent ".
Race to Dubai title might be only thing Justin Rose doesn't win Germany's Martin Kaymer (66) shared fourth with Lucas Bjerregaard (67) of Denmark, a shot further back. I was keenly aware I wanted to get back in the winner's circle and it was good to get it done today.
Cross Counter wins 2018 Melbourne Cup Flemington But the weather cleared after midday, buoying a festive crowd and drying out the track from heavy to soft an hour before the race. McEvoy timed Cross Counter's run perfectly after turning into the final straight well back in the field.
Supreme Court Rejects Net Neutrality Case It actually petitioned the Supreme Court to erase history and wipe out an earlier court decision upholding open internet policies. The Trump administration had warned that it would ask the high court to step in if the appeals court didn't rule by October 31.
Tobi Bakre honored at Prince Charles' 70th birthday in Ghana
Former Cowboy Dez Bryant agrees to deal with Saints
Caernarfon Town to host event with boxing star Tony Bellew next year
U.S. exempts India-backed port in Iran from sanctions
'She Has Earned This': Trump Praises Pelosi, Warns Democrats
Aussie airline aborts veterans-first boarding plan before takeoff
N. Korean leader likely to visit Russian Federation in November: S. Korean envoy
Morning people 'less likely to develop breast cancer'
PlayerUnknown's Battlegrounds (PUBG) coming to PS4 in December according to reports
Sri Lankan speaker refuses to accept Rajapakse as PM
Published: Thu, November 08, 2018
Worldwide | By Isabel Fisher
Democrats Capture US House Majority, Republicans Retain Control of Senate
Democratic incumbents also prevailed in Ohio, Pennsylvania and Wisconsin, Midwestern states that Trump carried narrowly two years ago.
But it remains to be seen whether Democrats' rage will amount to the so-called "blue wave" they've anticipated for almost two years, or whether it's even enough to gain the 23 seats needed to eke out a Democratic majority in the House.
Democrats could derail Trump's legislative agenda for the next two years should they win control of the House or the Senate.
A simple House majority would be enough to impeach Trump if evidence surfaces he obstructed justice or that his 2016 campaign colluded with Russian Federation.
As for Republicans retaining control of the Senate, she called it "a huge moment and victory for the president".
The midterms have seen a number of firsts in USA politics.
"We will have a responsibility to find our common ground where we can, stand our ground where we can't", Pelosi said.
"Tremendous success tonight", the president tweeted. He finished his final midterm campaign stretch on Monday with three rallies.
Historically, the party in power loses several seats during the first midterm election of a new president, particularly if his national job approval ratings are low.
Unless House Republicans can pressure enough moderate Democrats to vote with them, pro-life policy gains will again be limited to whatever changes to existing federal rules and regulations can be done by executive orders or directives to federal agencies.
US voters cast ballots on Tuesday to fill all 435 seats in the US House Representatives and approximately one-third of the 100-member US Senate in addition to other local and state offices.
While Sanders suggested Trump could blow off Pelosi in the wake of the midterms, she noted that the president is willing to work with whatever party ultimately ends up in power.
Pelosi has campaigned tirelessly this election season.
Djokovic drawn to face Zverev and Cilic in London — ATP Finals
They also held on to competitive seats in Texas, where Senator Ted Cruz fended off Representative Beto O'Rourke, the well-financed liberal darling, and in Tennessee, where Representative Marsha Blackburn prevailed.
Many of the Democratic candidates have military backgrounds and emerged as formidable challengers, particularly in red-state districts where Republicans have dominated. Of the three races he targeted in the final day, the Republicans won all of them: Mike Braun defeated Democratic Sen. Democrats also captured governorships in MI and IL. The president urged supporters to "pretend" he was on the ballot.
Democrats claimed some high-profile victories, with former professional hockey player Colin Allred defeating Pete Sessions, the chairman of the powerful House Rules Committee and leading opponent of legalized marijuana, in suburban Dallas.
The loss of the House is a serious blow to Trump who must now brace for the novel experience of oversight from Capitol Hill with Democratic committee chairmen promising constraints on his power that the GOP never attempted.
A record number of candidates identifying as "LGBT" ran for office this election cycle, and several of them will soon take office.
Democrats regained control of the House, while the GOP maintained control of the Senate.
But nonetheless, Republicans have been bracing for a loss in the House, though they anticipate keeping ahold of the Senate.
Tuesday night's results are a much-needed win for the Democrats, who have struggled in recent midterm elections.
Investors often favor Washington gridlock because it preserves the status quo and reduces uncertainty, even though many investors this time around had been hoping for a continuation of the Republican agenda.
Individual races "will be close", she said, but because of the "quality of our candidates" and emphasis on preserving health care, "I feel confident we will win".
But a US Department of Homeland Security official said the reports of voting technology failures appeared so far to have had no significant impact in preventing people from voting.
According to The New York Times, amid signs that the nation's deep political and cultural divisions that lifted Trump in 2016 may only be deepening, "rural voters were breaking sharply" with their counterparts in the suburban districts and metropolitan areas, as turnout soared in a midterm election that came to serve as a national referendum on the president. "And no matter what the outcome, whether you're a Republican or a Democrat, I think we can all agree that the big loser this year is all of our Thanksgiving dinners". In the last such congressional elections in 2014, there were 27.5 million early votes.
Health care was at the forefront of IN voters' minds, with nearly 3 IN 10 naming it as the most important issue facing the nation IN this year's midterm elections - including 30-year-old Cordell Chaney, who works at a Fort Wayne wire and cable products manufacturer.
Former Kenyan Refugee, Ilhan Omar Wins in US Elections in Minnesota
Liverpool lose their mojo to make Champions League last 16 a struggle
7-Eleven Pilots New 'Scan-And-Go' Checkout Technology
Veteran transfer will be x-factor in a Kentucky cover versus Duke
Bryan Cranston confirms 'Breaking Bad' movie in development
Pompeo Meeting With North Korean Officials Postponed - US State Department
Plzen Vs. Real Madrid Live Stream
Mysterious cigar-shaped interstellar object may be alien spacecraft: Harvard researchers
Net pioneer desires new 'contract' for web
French president target of planned attack, six arrested
US Attorney General Jeff Sessions resigns at Donald Trump's request
Dead brothel owner elected to legislative seat
Ariana Grande Knew Pete Davidson Would Mention Her On 'SNL'
Papa Gino's abruptly closes numerous pizzeria locations
Ariana Grande Sings "thank u, next" & Trips On Her Heels On 'Ellen'
Penguins detained in New Zealand after invading sushi bar
Chicago alligator 'Chance the Snapper' has finally been caught
New leak claims Trump scrapped Iran nuclear deal 'to spite Obama'

redpajama_set_name: RedPajamaCommonCrawl


text:
Arneberg Station (Arneberg stasjon) er en tidligere jernbanestation på Solørbanen, der ligger ved området Arneberg i Åsnes kommune i Norge.

Stationen blev oprettet som holdeplads, da banen mellem Kongsvinger og Flisa åbnede 3. november 1893. Den blev opgraderet til station 15. november 1916 og var bemandet som sådan indtil 1. august 1970. Persontrafikken på banen blev indstillet 29. august 1994.

Stationsbygningen, der var opført efter tegninger af Paul Due, blev revet ned 11. juli 1992. Ilgodshuset overlevede imidlertid, da det blev flyttet og genopført ved Lunderbye Nor i Kongsvinger, hvor der nu er kulturpark. I Arneberg er kun et af stationens tre spor farbart, mens de to andre er overgroede (status 2011).

Litteratur

Eksterne henvisninger

 Norske jernbanestasjoner om Arneberg Station

Stationer på Solørbanen
Jernbanestationer i Norge uden persontrafik
Etableret i 1893

redpajama_set_name: RedPajamaWikipedia


HPC partners with organizations that share our passion and commitment to improve the health of those in underserved communities. By partnering and collaborating we further expand our reach into the community helping those most at risk.
Want to Partner with HPC?
HPC seeks to align itself with people, organizations and community partners committed to helping those in underserved communities live healthier lives. With your help we can make this a reality. Go to the "How to help" section and enter your contact information at the "Partner with HPC" link.
Government - Strong governmental partners are essential to creating sustainable change. HPC partners with federal, state, and local government agencies through a variety of initiatives targeting individuals, organization, and systems. Our unique position as a trusted partner to both government entities and communities allows us to translate policy into practice at the community level, and to bring community voices to the policy development process.
Funders - HPC's work is significantly supported by federal, state, and local organizations, private foundations, and other institutions that seek to improve the health of individuals and communities disproportionately impacted by chronic disease and its risk factors. We reach out to leaders in the private sector to partner with us in an effort to expand the scope and reach of our programs and initiatives.
Community - HPC is a longstanding and trusted partner in the communities that we serve. Truly embedded in the communities that we serve, our staff has developed a deep understanding of the assets that each community possesses, and the challenges that each faces. We view communities as partners in creating and sustaining changes that support healthy lives. With this in mind, HPC serves as a bridge between many of its partners by representing and bringing community voices to tables where decisions are made, and by translating theory and policy into practice at the community level.


At Severn Utilities Valves we offer an excellent range of air release valves for most applications. We have single, double and triple function versions in Ductile Iron GGG50 with Stainless Steel and Aluminium Bronze Trim suitable for both clean water and sewage applications. All products are produced in accordance with BS EN 1074-4 at PN10/16/25/40 pressure rating in sizes DN40 to DN500.


I have experience nannying and babysitting multiple children 0-4 years old. I am CPR and first aid certified for infant and adult. Also, I have experience tutoring 2nd through 8th grade in Math and Reading in Chicago public Schools and provide summer academic support for older children.


Made from heavyweight cotton twill, these 'Leaf' or 'Duck Hunter' camouflaged trousers have two exposed button hip pockets, two exposed button thigh cargo pockets and a small first aid pocket on the left leg. They are also equipped with leg bottom drawstrings and a button fly. This was one of two leaf camouflage patterns known to have been issued by CISO to Special Forces and CIDG strike teams operating in the Mekong Delta area.
U.S. COTTON DUCK CANVAS DUFFEL BAG OLIVE GREEN VIETNAM WAR ERA Detroit Mich.


text:
Surname: Coe
William Wilson, the pioneer ancestor of this family, emigrated from Stewardstown, County of Tyrone, Ireland, in 1732, when 19 years of age. The Town of Stewardstown is in the parish of Donagheny in the province of Ulster and eighty-two miles northwest of Dublin, long noted for its very superior linen cloth.
Ancestry of Henry Huttleston Rogers of Fairhaven Massachusetts
Henry Huttleston Rogers, Fairhaven's most distinguished son, was born there Jan. 29, 1840, and died May 19, 1909, in New York City. Of typical New England stock and Old Colony antecedents, his continued identity with Fairhaven made him dearly beloved in that community. The Rogers family is, perhaps, one of the most ancient and numerous of the old settled families in the country. There were no less than a dozen who bore the name of John Rogers among the seventeenth century emigrants, and one of this Christian name was president of Harvard College in the latter part of that century. It is the purpose in this article to deal, briefly, with only one of the New England Rogers families – that of which Henry Huttleston Rogers was a representative.
Index to Articles found in the El Farol Newspaper 1905-1906
The Lincoln County New Mexico online archives contains pdf's of all remaining copies of the El Farol Newspaper of Capitan NM, but doesn't have an index to the newspaper. C. W. Barnum, an active member of AHGP, and state coordinator for the New Mexico AHGP recently invested his time and energy into providing an every person index to the various extant issues. He has shared this wonderful index with AccessGenealogy in hopes that it will reach a wider audience. Enjoy!
1923 Historical and Pictorial Directory of Angola Indiana
Luedders' historical and pictorial city directory of Angola, Indiana for the year 1923, containing an historical compilation of items of local interest, a complete canvass of names in the city, which includes every member of the family, college students, families on rural lines, directory of officers of county, city, lodges, churches, societies, a directory of streets, and a classified business directory.
Portrait and Biographical Record of Seneca and Schuyler Counties, NY
In this volume will be found a record of many whose lives are worthy the imitation of coming generations. It tells how some, commencing life in poverty, by industry and economy have accumulated wealth. It tells how others, with limited advantages for securing an education, have become learned men and women, with an influence extending throughout the length and breadth of the land. It tells of men who have risen from the lower walks of life to eminence as statesmen, and whose names have become famous. It tells of those in every walk in life who have striven to succeed,
Seneca County New York Biographies
In the 1980's a series of newsletters were published four times a year by Seneca County NY featuring historical information concerning Seneca county and her past residents. The current historian for Seneca County placed these online using PDF files. One of the main features of each edition were biographical sketches of early settlers of Seneca County. Unfortunately, while they provided an index inside of a spreadsheet for the 189 biographies, it is difficult for the average user to quickly get around. I've taken their spreadsheet and linked each edition to the PDF file. Once you've found the biography you want,
1894 Michigan State Census – Eaton County
United States Soldiers of the Civil War Residing in Michigan, June 1, 1894 [ Names within brackets are reported in letters. ] Eaton County Bellevue Township. – Elias Stewart, Frank F. Hughes, Edwin J. Wood, Samuel Van Orman, John D. Conklin, Martin V. Moon. Mitchell Drollett, Levi Evans, William Fisher, William E. Pixley, William Henry Luscomb, George Carroll, Collins S. Lewis, David Crowell, Aaron Skeggs, Thomas Bailey, Andrew Day, L. G. Showerman, Hulbert Parmer, Fletcher Campbell, Lorenzo D. Fall, William Farlin, Francis Beecraft, William Caton, Servitus Tucker, William Shipp, Theodore Davis. Village of Bellevue. – William H. Latta, Thomas B.
Genealogy of Aaron French, Jr.
2 AARON FRENCH, Jr. (Aaron1), b. Apr. 19, 1767, Essex Co., N. J.; d. Jan. 31, 1850, Johnstown, O.; m. (1st), Mar. 8, 1792, Washington Co., Pa., Ruth Coe (b. Aug. 19, 1770, Morristown, N. J.; d. Mar. 19, 1835, Johnstown, O.), dau. of Elder Joseph Coe (Joseph, Joseph, Benjamin, Robert), and Abigail Moon, his w. Aaron French 2 m. (2nd) Oct. 8, 1835, Catharine Combs (d. Aug. 9, 1856), wid. of – Starkey. Robert Coe, ancestor of Ruth (Coe) French, came to Mass., 1634, from Suffolkshire, England, where he was b., 1596. Children of first marriage (none of second):
Coe, Lee Ellen – Obituary
Lee Ellen Coe, 79, of Elgin, died Aug. 2, 1993, at Valley View Care Center in La Grande. A memorial service will be held at 1 p.m. on Saturday at the Church of Jesus Christ of Latter-day Saints in Elgin. Mrs. Coe was born Nov. 5, 1913, in Elgin, to William and Alma Long Breshears. She graduated from Cove High School when she was 15. She then attended the University of Oregon and graduated when she was 18. She farmed at Pine Grove and Cricket Flats. She cooked for the farm crews. After this she got her teaching certificate and
Coe, Harhsley – Obituary
Union, Oregon Funeral Services for Hashley Coe are scheduled for Thursday, Sept. 14 at 2 p.m. Details will be given by Crippin & Daniels Funeral Home when completed. The La Grande Observer – Tuesday, September12, 1967


text:
Courts 14
1 year ago Featured, Hill Country NewsCoronavirus, courts, Greg Abbott, Health Care, higher education, public education, Texas Government, Texas News, Texas Policy, Texas Politics
Texas schools can again set their own face mask rules after federal judge overrules Gov. Greg Abbott's ban
BY BRIAN LOPEZ at The Texas Tribune, NOV. 10, 2021 Sign up for The Brief, our daily newsletter that keeps readers up to speed on the most essential Texas news. A federal judge ruled Wednesday that Gov. Greg Abbott's executive order prohibiting mask mandates in schools violates the Americans with Disabilities Act — freeing local officials to […]
1 year ago Featured, Hill Country Newscourts, criminal justice, death penalty, Texas Department Of Criminal Justice, Texas Government, Texas News, Texas Policy, Texas Politics, Texas prisons, U.S. Supreme Court
U.S. Supreme Court justices appear reluctant to loosen restrictions on religious advisers during Texas executions
BY JOLIE MCCULLOUGH NOV. 9, 2021 Sign up for The Brief, our daily newsletter that keeps readers up to speed on the most essential Texas news. The U.S. Supreme Court debated Tuesday whether the pastor of a Texas prisoner should be able to touch or audibly pray over him as the prisoner is executed. The justices largely […]
1 year ago Featured, Hill Country Newscourts, criminal justice, death penalty, Texas Department Of Criminal Justice, Texas Government, Texas Policy, Texas Politics, U.S. Supreme Court
U.S. Supreme Court weighs religion's place in the Texas death chamber
BY JOLIE MCCULLOUGH at The Texas Tribune, NOV. 9, 2021 Sign up for The Brief, our daily newsletter that keeps readers up to speed on the most essential Texas news. The U.S. Supreme Court is set to hear arguments Tuesday on the religious rights of those condemned to die in Texas. The justices, who have taken a […]
1 year ago Featured, Hill Country Newscourts, criminal justice, Department of State Health Services, Marijuana, state government, Texas Government, Texas News, Texas Policy, Texas Politics
Delta-8 is legal in Texas — for now — after Travis County judge blocks state from criminalizing the cannabis extract
BY KEVIN REYNOLDS at The Texas Tribune, NOV. 8, 2021 Sign up for The Brief, our daily newsletter that keeps readers up to speed on the most essential Texas news. Delta-8, the popular cannabis extract that was recently and suddenly outlawed in Texas, is temporarily legal again. State district court Judge Jan Soifer on Monday granted […]
1 year ago Featured, Hill Country News87th Legislative Session, courts, elections, Politics, state government, Texas Government, Texas Policy, Texas Politics, voting, Voting Rights Act
Justice Department sues Texas over new voting law, targeting restrictions on mail-in ballots and voter assistance
BY CASSANDRA POLLOCK at The Texas Tribune, NOV. 4, 2021 Sign up for The Brief, our daily newsletter that keeps readers up to speed on the most essential Texas news. Disabled, elderly and non-English speaking voters risk disenfranchisement under Texas' new voting law passed by the GOP-controlled Legislature earlier this year, the U.S. Department of Justice claims […]
1 year ago Featured, Hill Country Newscourts, criminal justice, Greg Abbott, immigration, Law Enforcement, Politics, Texas Government, Texas Policy, Texas Politics
In latest blunder, charges dropped against migrants arrested in Texas governor's border crackdown because of faulty paperwork
BY JOLIE MCCULLOUGH at The Texas Tribune, NOV. 4, 2021 Sign up for The Brief, our daily newsletter that keeps readers up to speed on the most essential Texas news. Trespassing charges filed against dozens of migrants arrested under Gov. Greg Abbott's "catch and jail" border security initiative were dropped last week because court documents filed by […]
1 year ago Featured, Hill Country News87th Legislative Session, courts, demographics, elections, Politics, redistricting, Republicans, state government, Texas Government, Texas Legislature, Texas Policy, Texas Politics, voting
Texas' new House map challenged in state court, expanding redistricting fight
BY ALEXA URA at The Texas Tribune, NOV. 3, 2021 Sign up for The Brief, our daily newsletter that keeps readers up to speed on the most essential Texas news. Opening a second front in widening legal wars over redistricting, a coalition of mostly Hispanic, Democratic members of the Texas House filed suit in state court Wednesday […]
1 year ago Featured, Hill Country Newsabortion, courts, gun rights, Health Care, Politics, Texas Government, Texas Policy, Texas Politics
Abortion providers and gun rights advocates are "strange bedfellows" in fight to strike down Texas' new abortion law
BY REESE OXNER AND JAMES BARRAGÁN at The Texas Tribune, NOV. 2, 2021 Sign up for The Brief, our daily newsletter that keeps readers up to speed on the most essential Texas news. Abortion-rights advocates have found an unexpected ally in their fight to overturn Texas' controversial abortion law: gun rights advocates, fearful that the same novel mechanism employed […]


Nice job! Well done and well said. First and formost there are all the components of concern that you mentioned regarding safety and finances and so on, but just as big…the cross-cultural differences. You have experience with this culture are well traveled and culturally competent. Going to the family like you did especially with this culture was nice and respectful. I didn't think about this whole family aspect when I thought about all your guys' adventures and bold moves that many date to consider. Brave!
*sigh*…."Anyway you talk a lot" LOL.. I trust you'd of have all the right words to conform the fam.
You chose a big wedding as the time to break the big news? Brave move, Bjorn ! You ran the risk of either taking advantage of the happy mood spilling over to you, or sucking the happiness out of the entire day ! Hah!
Stressful family discussions – I've had plenty of em. And I'm with you 100% – you can't predict what they'll say, but best to do your homework by preparing answers to objections. And learn to sell !
Razwana recently posted…MORE taglines. Are you kidding me?
Kind words, cousin:) The look was priceless..
Congratulations! Being a Filipino myself and having been raised with Filipino family values, I imagine that must have been difficult.
Cheers to your great adventure!
I know!! The amount of conversations I wish I had not put off!! Much love to the two of you..
Awesome job! See all the benefits of your travels and even the benefits for your zoo-loving Filipino father-in-law who was able to visit you overseas. If you were able to crush this fear, you could swim with sharks in Bali, right!!?
Our reality is often much much bigger than our fears. A good reminder that you have to face your fears to live your dreams.
p.s Did you have medical professionals around when making this announcement ?
Good approach to cracking difficult and potentially hazardous news. Interesting that you tried them on us first. We are pleased that things have gone well so far and wish you and Jammie a very good and rewarding future.
Heya now i am the first time below. I ran across the following mother board so i to locate It truly useful & the idea solved the problem available a lot. I'm hoping to supply a thing once more along with help other folks just like you taught me to be.
I am going to without delay clutch system your rss feed after i are not able to find your own e-mail membership weblink or maybe e-zine service. Conduct you might have any kind of? Please i want to know so I'll signed up. Many thanks.


Our generators including silent generators, open generators, ats generators, trailer generators. 3.We offer the spare parts for our generators all the time,any time you can contact us for spare parts. Make the generator more safe during the transportation time.
4 YRS Jiangsu Quanchang Airpower Co., Ltd.
50Hz / 60Hz Power Factor. 50Hz / 60Hz Power Factor. 0.8 Voltage Regulator.
4 YRS Fuan Longkai Power Co., Ltd.
5 YRS Taizhou Lvyang Garden Machine Co., Ltd.
Further post treatment after the RO system such as mixed bed deionization can increase the quality of the RO permeate and make it suitable for the most demanding applications. Activated Carbon Filter GAC(granular actitavted carbon) is used for both removing organic constituents and residual disinfectants (such as chlorine and chloramines) from water. Water softener A water softener can be used to help prevent scaling in an RO system by exchanging scale forming ions with non scale forming ions.
Alibaba.com offers 3,843 fresh generator products. About 1% of these are diesel generators, 1% are gas generation equipment, and 1% are alternative energy generators.
A wide variety of fresh generator options are available to you, such as ce, rohs, and gs. You can also choose from hot & cold, activated carbon air filter, and ozone generator. As well as from oxygen, nitrogen, and water. And whether fresh generator is free samples, or paid samples.
There are 3,843 fresh generator suppliers, mainly located in Asia. The top supplying country is China (Mainland), which supply 100% of fresh generator respectively.
Fresh generator products are most popular in Southeast Asia, Mid East, and North America.
You can ensure product safety by selecting from certified suppliers, including 2,014 with ISO9001, 277 with Other, and 229 with ISO14001 certification.


text:
Q: Error while exporting spark sql dataframe to csv I have referred the following links in order to understand how to export spark sql dataframe in python

*

*https://github.com/databricks/spark-csv

*How to export data from Spark SQL to CSV
My code:
df = sqlContext.createDataFrame(routeRDD, ['Consigner', 'AverageScore', 'Trips'])
df.select('Consigner', 'AverageScore', 'Trips').write.format('com.databricks.spark.csv').options(header='true').save('file:///opt/BIG-DATA/VisualCargo/output/top_consigner.csv')

I load the job with spark-submit passing the following jars on master url
spark-csv_2.11-1.5.0.jar, commons-csv-1.4.jar

I am getting the following error
df.select('Consigner', 'AverageScore', 'Trips').write.format('com.databricks.spark.csv').options(header='true').save('file:///opt/BIG-DATA/VisualCargo/output/top_consigner.csv')
      File "/opt/cloudera/parcels/CDH-5.5.1-1.cdh5.5.1.p0.11/lib/spark/python/lib/pyspark.zip/pyspark/sql/readwriter.py", line 332, in save
      File "/opt/cloudera/parcels/CDH-5.5.1-1.cdh5.5.1.p0.11/lib/spark/python/lib/py4j-0.8.2.1-src.zip/py4j/java_gateway.py", line 538, in __call__
      File "/opt/cloudera/parcels/CDH-5.5.1-1.cdh5.5.1.p0.11/lib/spark/python/lib/pyspark.zip/pyspark/sql/utils.py", line 36, in deco
      File "/opt/cloudera/parcels/CDH-5.5.1-1.cdh5.5.1.p0.11/lib/spark/python/lib/py4j-0.8.2.1-src.zip/py4j/protocol.py", line 300, in get_return_value
    py4j.protocol.Py4JJavaError: An error occurred while calling o156.save.

py4j.protocol.Py4JJavaError: An error occurred while calling o156.save.
    : java.lang.NoSuchMethodError: scala.Predef$.$conforms()Lscala/Predef$$less$colon$less;
        at com.databricks.spark.csv.util.CompressionCodecs$.<init>(CompressionCodecs.scala:29)
        at com.databricks.spark.csv.util.CompressionCodecs$.<clinit>(CompressionCodecs.scala)
        at com.databricks.spark.csv.DefaultSource.createRelation(DefaultSource.scala:198)
        at org.apache.spark.sql.execution.datasources.ResolvedDataSource$.apply(ResolvedDataSource.scala:170)
        at org.apache.spark.sql.DataFrameWriter.save(DataFrameWriter.scala:146)
        at org.apache.spark.sql.DataFrameWriter.save(DataFrameWriter.scala:137)
        at sun.reflect.NativeMethodAccessorImpl.invoke0(Native Method)
        at sun.reflect.NativeMethodAccessorImpl.invoke(NativeMethodAccessorImpl.java:62)
        at sun.reflect.DelegatingMethodAccessorImpl.invoke(DelegatingMethodAccessorImpl.java:43)
        at java.lang.reflect.Method.invoke(Method.java:498)
        at py4j.reflection.MethodInvoker.invoke(MethodInvoker.java:231)
        at py4j.reflection.ReflectionEngine.invoke(ReflectionEngine.java:379)
        at py4j.Gateway.invoke(Gateway.java:259)
        at py4j.commands.AbstractCommand.invokeMethod(AbstractCommand.java:133)
        at py4j.commands.CallCommand.execute(CallCommand.java:79)
        at py4j.GatewayConnection.run(GatewayConnection.java:207)
        at java.lang.Thread.run(Thread.java:745)

A: Spark version 1.5.0-cdh5.5.1 is built with Scala 2.10 - default Scala version for Spark < 2.0. Your spark-csv is built with Scala 2.10 - spark-csv_2.11-1.5.0.jar.
Please update spark-csv to version with Scala 2.10 or update Spark to Scala 2.11. You will know Scala version by number after artifactId, i.e. spark-csv_2.10-1.5.0 will be for Scala 2.10

A: I am running Spark on Windows and I faced the similar issue of not able to write to file(CSV or Parquet). Upon reading more into Spark website, I found the below error, and it is because of the winutils version that I am using. I changed it to 64bit and it worked. Hope this helps some one.
Spark Log

redpajama_set_name: RedPajamaStackExchange


Resources for the BASIC Stamp 2 microcontroller including the Stamps in Class series.
What are control systems and how can they be used with the BASIC Stamp 2? Check out this in-depth tutorial to find out!
Get started with basic circuits and programming! What's a Microcontroller? is a fun and engaging introductory text for the BASIC Stamp microcontroller and Board of Education, or BASIC Stamp HomeWork Board.
Read more about What's A Microcontroller?
Build your own robot, wire it up with sensors, and let it roam on its own. Robotics with the Boe-Bot includes step-by-step assembly instructions, circuit-building, and programming for the BASIC Stamp-based Boe-Bot Robot.


Patryk is a Polish antifascist recently deported to Poland from UK to serve his sentence from 11 years ago for allegedly assaulting some fash. He would appreciate your letters of support and literature, he understands Polish and English well. We are also still collecting money to support his son that stayed in UK and is living with his brother. Address can be published as well.


Pokies machine Fruits of Ra, developed by Globotech, please lovers and juicy fruit, and ancient Egypt. The online pokies Fruit Ra profitable to play for real money with a stable payments. But if you want each player can at any time run the free version.
Here are 5 reels and 5 paylines as in Sizzling Hot Deluxe. There is a Wild symbol and a Scatter. There is a risk game, allowing each to increase their winnings repeatedly. The machine Fruits of Ra prize combination even count right to left.
Most of the pictures, presented in the online pokies, as can be understood from the game title, fruit. There is also a five-pointed star image is a symbol of Scatter. Its location on the drums does not matter, important only to the number of fallen stars. Depending on the total amount they multiply rate of from 5 to 100 times. Emblem of the Wild scarab represented. It replaces other icons except for the scatter symbol. The greatest gains in the gaming machine Fruits of Ra bring Red Seven. If a picture with her completely fill the active line, the rate on it is multiplied 5,000 times. The wild symbol will help more profitable to play Polar Fox for real money. In it, the role of Wild went to the polar fox with coefficients up to 9000.
Each prize obtained in the main online slots game Fruits of Ra can be increased several times in the risk game. In it the player will be offered two options: to guess the color of the closed card or her suit. In the first case, the correct answer winnings will be doubled in the second - four. And in the mode of doubling in the Police Story, you need to guess the cards with valuable evidence.
In the risk game machine Fruits of Ra can you can test your strength several times, and each correct guess will increase the current payment. But at the first failure, the money "will be burned".


text:
\section{\label{sec:level1}Introduction\protect\\
}
The Stern-Gerlach experiment provided an evidence for existence of spin as an intrinsic, non-classical property [1]. A beam of silver atoms traveling through an inhomogeneous magnetic field is deflected up or down depending on their spin. Strangely, this experiment did not work with beams of electrons [2]. Bohr and Pauli emphasized, free electrons cannot be spin-polarized by exploiting magnetic fields, because of the combined effects of the Lorentz force and quantum uncertainty principle. This conclusion was due to the concept of classical particle trajectories and became a general argument in scientific literature [3-5].

One of the first efforts refuting the Bohr and Pauli's statement was using a longitudinal magnetic-field configuration instead of the standard transverse geometry of Stern-Gerlach. In this way, the complete spin splitting with quantum-mechanical analysis has been reported [6-9]. In recent theoretical studies, the use of the grating and electromagnetic fields are resulted in the spin separation for electrons. Tang proposed a spin-polarized Talbot effect which is  non-paraxial for an electron beam scattered from a grating of magnetic nanostructures [10]. Also a transverse Stern-Gerlach magnet which diffracts electrons by a magnetic phase grating was discussed by McGregor \textit{et al} [11]. They indicated that by applying a current to the solenoids, a spin-dependent phase difference is created between the two arms of the Mach-Zehnder interferometer [12]. Moreover, a novel space-variant Wien filter, named "q-filter", which is composed of space variant orthogonal electric and magnetic fields can act as an efficient spin-polarization filter. This filter couples spin angular momentum to orbital angular momentum for electron, neutron, or atom beams [13-14].

Kapitza-Dirac (KD) effect, the quantum mechanical diffraction of an electron on a periodic spatial structure formed by a standing light wave, confirmed that it could be a way to detect the spin of electrons [15]. Ahrens \textit{et al.} theoretically showed complete spin-flip transitions applying relativistic treatment for KD effect [16-17]. It was demonstrated that electrons according to their spin state in the interaction with circularly polarized counter-propagating monochromatic standing waves can be separated [18]. In the meantime, Dellweg \textit{et al}. reported a similar way of generating spin-polarized electrons by using bichromatic ($\omega$:$2\omega$) laser beams in Kapitza-Dirac effect [19-20]. Also Dellweg showed that spin dynamics of electrons in bichromatic KD effect is dependent on the polarization of laser beams and therefore the spin direction of the output beams can be controlled [21-22].

One major result of these studies is that the initial electron with spin up state is transferred to the scattered electron with spin down and vice versa. This is symmetric flipping spin dynamics. For especial two cases, circularly polarization in KD effect with equal frequency [18] and combination of linear-circular polarization in bichromatic KD effect with a frequency ratio of 2  [22] the spin of electron does not flip and preserves its state.

In the present paper, we theoretically discuss bichromatic KD effect arising from the interaction of the laser beam with frequency of $\omega$ and the counter-propagating laser beam with frequency of $3\omega$. In these fields, the electron exchanges four photons and the four-photon bichromatic KD (4PBKD) occurs. We investigate the spin polarization of the electron using various polarized counter propagating lasers beams with a frequency ratio of three. We focus on the electron whose momentum is parallel to the laser beam axis so that the interaction term $ \vec{p}.\vec{A} $ becomes very insignificant. Our article is organized as follows: in Sec. II we determine that in bichromatic standing waves with a frequency ratio of 1:3, electron exchanges four photons. Then based on the $ \textit{S} $ matrix approach, transition amplitude for resonant state is calculated and polarization dependent Rabi frequency is taken into account. Numerical solutions of the time-dependent Dirac equation in momentum space are applied to clear up relativistic quantum dynamics in Sec. III and look into scattering probability result of the different polarizations of two-color beams. In this paper atomic units are used throughout unless otherwise stated.

\section{Theoretical Description}
\subsection{\label{sec:level2}Electron Dispersion in Bragg Regime}
The interaction between an electron and two counter-propagating laser fields of frequency $ \omega_i(i=1,2)$ is due to the absorption of some photons from laser beam 1 and the  stimulated emission of some photons to laser beam 2. In the case of an intense bichromatic standing wave, the multiphoton interaction between electron and laser field becomes more likely. The absorption of $ N_a $ photons with $ \omega_1 $ frequency and emission of $ N_e $ photons with $ \omega_2 $ frequency conserve energy and momentum if $N_a\omega_1=N_e\omega_2$. In case of $ \omega_1=\omega $ and $ \omega_2=3\omega $, a free electron absorbs three  $ \omega $ photons and emits one $ 3\omega $ photon or vice versa. Since a photon has the energy $ c \hbar k  $ and the momentum $\hbar k  $, the total transferred energy is  $\triangle E=c (N_a k_1-N_e k_2) $ and the total transferred momentum is $ \triangle p= (N_ak_1+N_ek_2) $. In the presence of the fundamental frequency and the third harmonic with $ N_a=3$ and $N_e=1$, after the interaction the electron momentum change is $ 6k $.

The relativistic energy-momentum relation secant and quantum pathway that increases electron momentum by $ 6k $ are shown in Fig. 1. The total exchange of energy and momentum of the electron with laser beams is represented by horizontal dash line.
This slop is given by $ s=\frac{\triangle E}{\triangle p} $ and connects initial and final momenta of diffracted electron [17].
All pathways in Bragg regime starts and ends exactly on the dispersion relation secant. Theoretically, other transitions are also possible as well, but we focus on the resonant two-state quantum dynamics in Bragg regime. Absorption of one photon of $ 3\omega $ and emission of three photons of $ \omega $ make no difference in result.
\begin{figure}
\resizebox{86mm}{68mm}{\includegraphics{dispersion}
\begin{picture}(0.8,0.6)
\put(-14,25) {$\dfrac{p}{mc^2}$}
\end{picture}
\begin{picture}(0.7,0.1)
\put(5,200) {$\dfrac{\varepsilon(p)}{mc^2}$}
\end{picture}
\caption{\label{fig:epsart} Sketch of dominant pathway of four-photon KD effect in bichromatic standing waves. The dispersion relation of energy and momentum is in Bragg regime and each wiggly arrow shows a photon.}
\end{figure}
\subsection{\label{sec:level2}\textit{S} Matrix Approach}

The evaluation of the relativistic electron in four-photon Kapitza-Dirac process is described quantum mechanically by Dirac equation
\begin{equation}
\left(
i\hbar\slashed{\partial}+\dfrac{e}{c}\slashed{A}(x)-m
 \right)\psi(x)=0,
\end{equation}
 in which $\slashed{A}  $ is denoted by Feynman slash $ \slashed{A}=\gamma.A $  and $\gamma$ stands for Dirac matrices.

  An analytical treatment for multiphoton stimulated Compton scattering such as bichromatic Kapitza-Dirac scattering has been accomplished through $ \textit{S} $ matrix approach with suitable approximations [22]. The Dirac equation has a well known solution; Volkov state for an electron in the case of the external potential being a plane wave. By using the fundamental laser mode and Volkov sates for the incident electron, the remaining four-photon Kapitza-Dirac process can be represented within the first order perturbation theory [23-24]. The calculation of S matrix is the same as that used in three photons KD effect, except that a further photon participates in the interaction.

In the presence of third harmonic the $ \textit{S} $ matrix for transition from $ p $ to $ p^\prime $ by absorbing three photons from $ A_1 $ as beam with fundamental frequency and emitting one photon into $ A_2 $ as beam with $ 3\omega$ frequency is given by
  \begin{eqnarray}
    S &\approx& \frac{ie}{cV} \int d^4x\, \bar{u}_{p', s'} \Bigg(
     \slashed{A}_2^{(+)} \tilde{J}_2 e^{i \left( p' - p - 3k_1 \right) \cdot x} \nonumber\\
     & & \left. - \frac{e}{2 c} \left[ \frac{\slashed{A}_1^{(-)} \slashed{k} \slashed{A}_2^{(+)}}{k_1 \cdot p'} + \frac{\slashed{A}_2^{(+)} \slashed{k}_1 \slashed{A}_1^{(-)}}{k_1 \cdot p} \right]
     \tilde{J}_1 e^{i \left( p' - p - k_1 \right) \cdot x}
     \right) u_{p, s} \nonumber\\
     &\approx& \frac{i e}{2} T \bar{u}_{p', s'} \left[
      a_2 \tilde{J}_2 \bar{\slashed{\epsilon}}_2
     - \frac{e a_1 a_2}{4 c} \tilde{J}_1 \left( \frac{\slashed{\epsilon}_1 \slashed{k}_1 \bar{\slashed{\epsilon}}_2}{k_1 \cdot p'}
      + \frac{\bar{\slashed{\epsilon}}_2 \slashed{k}_1 \slashed{\epsilon}_1}{k_1 \cdot p} \right)
     \right] u_{p, s}. \nonumber\\

  \end{eqnarray}
  Here, $\slashed{A}_1^{(-)} = \frac{1}{2} a_1 \slashed{\epsilon}_1 e^{-i k_1 \cdot x}$ is the component that defines the absorption of one photon from $ A_1 $, and  $\slashed{A}_2^{(+)} = \frac{1}{2} a_2 \bar{\slashed{\epsilon}}_2 e^{i k_2 \cdot x}$  where $\bar{\slashed{\epsilon}}_2=\epsilon_2^*\cdot\gamma$ is the component that describes emission of one photon into $ A_2 $. Also $ \tilde{J}_{1,2}$ are generalized Bessel functions. In this derivation only resonant scattering process was considered, which fulfilled the Bragg condition. Therefore the $d^4x$- integration does result in the factor $c VT $, with $ T $ the interaction time and $ V$ quantification volume [22]. The initial and scattered electron momentum is set respectively to $p=(p^0,p_x,0,-3 \hbar k)$ and $p^\prime=(p^0,p_x,0,+3 \hbar k)$. The Dirac spinors for theses momenta are corresponding to Pauli spinors by
 \begin{equation}
u_{(p,s)}=\frac{1}{\sqrt{2mc(p^0+mc)}}\quad \begin{pmatrix}
(p^0+mc)\chi_s \\
\vec{p}.\vec{\sigma}\chi_s
\end{pmatrix}.
\quad
\end{equation}
  We can calculate a part of Eq. (2) as
\begin{equation}
   \left( \bar{u}_{p', s'} \bar{\slashed{\epsilon}}_2 u_{p, s} \right)_{s', s}
    = -\frac{p_x}{m c} \vec{\epsilon}_2^{~*} \cdot \vec{e}_x + i \frac{3\omega}{m c^2} \left( \vec{\epsilon}_2^{~*}\times\vec{e}_z \right)\cdot \vec{\sigma}
  \end{equation}
  and in a similar way
  \begin{eqnarray}
    & & \left( \bar{u}_{p',s'}\left[
     \frac{\slashed{\epsilon}_1 \slashed{k}_1 \bar{\slashed{\epsilon}}_2}{k_1 \cdot p'} + \frac{\bar{\slashed{\epsilon}}_2 \slashed{k}_1 \slashed{\epsilon}_1}{k_1 \cdot p}
    \right] u_{p,s} \right)_{s', s} \nonumber\\
 &\approx& \dfrac{2 \vec{\epsilon}_1 \cdot \vec{\epsilon_2^{~*}}}{m c}
    + \frac{6 i \omega}{m^2 c^3} \left( \vec{\epsilon}_1 \times \vec{\epsilon_2}^{*} \right)\cdot \vec{\sigma}.
  \end{eqnarray}
 Also from the Taylor series of the generalized Bessel functions, we can estimate
   \begin{eqnarray}
   \tilde{J}_1 \approx -3\frac{e a_{1}}{m c^2} \frac{p_{x}}{m c} \vec{\epsilon_1} \cdot \vec{e_x}, \nonumber\\
   \tilde{J}_2
   \approx \frac{e^2 a_1^2}{m^2 c^4} \left( \frac{36}{8} \frac{p_x^2}{m^2 c^2} \left( \vec{\epsilon_1} \cdot \vec{e_x} \right)^2 - \frac{3}{8}\vec{\epsilon}_1^{~2} \right).
  \end{eqnarray}
  Putting all this together, the $ \textit{S} $  matrix of Eq. 2 for small transverse momentum is estimated as follows
\begin{eqnarray}
& S\approx \dfrac{i}{2} T\dfrac{e^{3}a_1^{2}a_2}{m^{3}c^{6}}\left[
\dfrac{3}{8\hbar}p_x c \vec{\epsilon_1}^{2} \vec{\epsilon_2}^{*} .\vec{e_x}+
\dfrac{3}{4\hbar}p_x c \vec{\epsilon_1}.\vec{e_x} \vec{\epsilon_1}.\vec{\epsilon_2}^{*} \right.\nonumber\\
 &\left. -\dfrac{9i}{8}\omega \vec{\epsilon_1}^2
 (\vec{\epsilon_2}^{*}\times\vec{e_z}). \vec{\sigma}\right]
  =\dfrac{i}{2}T\xi_1^2\xi_2\hat{\Omega}.
\end{eqnarray}
Here $ \xi_{1,2}=\dfrac{ea_{1,2}}{mc^2}$ are the common dimensionless field amplitudes used in atomic physics. It is clear that for electrons entirely on $ z $ axis, the transition from $ p $ to $ p^\prime $ is dependent on the polarization beam vectors $  \vec{\epsilon_i} $ and the direction of electron spin along $z$ axis.
Generally for combination of the fundamental laser beam with higher harmonics laser beam, $ \hat{\Omega} $ has the common form presented in Eq. 7 and just the coefficients of each term are changed. For the electron with $ p_x=p_y=0 $, the third term of Eq. 7 has an essential role in the spin state of the scattered electron. As a result, we expect that the electron parallel to the beam axis in bichromatic ($\omega$:$3\omega$) laser beams shows the similar spin dynamics behavior as in bichromatic ($\omega$:$2\omega$) standing waves.

\section{Numerical Results}
In this section, the numerical results will be presented for the spin-dependent Kapitza-Dirac scattering in bichromatic counter-propagating laser fields with a frequency ratio of 3. Taking into account the combined vector potential and rewriting Dirac equation in momentum space, we find a system of coupled ordinary differential equations. The numerical solution of differential equations is obtained by employing a Crank-Nicholson scheme. The solutions are the absolute square values of the expansion coefficients that represent scattering probability of the electron in the particular quantum state. $ c_n^{\zeta}(n=0,\pm1,\pm2,...)$ coefficients represent electrons with momentum $p_n=(p_x,0,nk)$. The index $ \zeta\in\lbrace+\uparrow,+\downarrow,-\uparrow,-\downarrow \rbrace$ labels the sign of the energy and the spin direction. These states can be denoted by $\vert nk,\zeta\rangle $.

In the four-photon KD effect, the vector potential for the bichromatic field $ (\omega:3\omega) $ can be described in the form of
\begin{equation}
\vec{A} =A_1\left[\cos (k(z\pm ct))\hat{\epsilon}_1\right]+A_2\left[\cos (3k(z\pm ct))\hat{\epsilon}_2\right],
\end{equation}
where $A_1$ and $A_2 $ are the amplitudes of standing waves and $\epsilon_1$ , $\epsilon_2$ are polarization vectors. The electron with initial longitudinal momentum of $p_z=-3k $ in presence of the mentioned vector potential is scattered into mirror mode with longitudinal momentum $p_z=+3k $ by exchanging $ 6k $  momentum. For all next calculations, we start with longitudinal momentum $p_z=-3k $ and spin projection either up or down, while the other momenta modes at initial time will be zero. As mentioned in Bragg regime, transfer of population is restricted to $p_z= +3k $ for the final state and occupation probability of other momenta modes is very small. When the electron has component perpendicular to laser beam direction, all four states $\vert-3,+\uparrow\rangle $, $\vert-3,+\downarrow\rangle$, $\vert+3,+\uparrow\rangle $ and $\vert+3,+\downarrow\rangle $ participate in the interaction. It is worth noting that because of focusing on the effect of $\vec{\sigma}.\vec{B}$ in this work, we choose electron momentum to be parallel to the axis of the laser beam, however practically the influence of $ \vec{p}.\vec{A} $ cannot be ignored.

In all simulations, smooth switching on and off laser fields are $sin^2 $ slopes for five cycle laser periods with a flat top function. To study spin effects in four-photon KD diffraction, the following various polarizations of this bichromatic standing wave are considered:
\begin{figure}[t]
\resizebox{86mm}{68mm}{\includegraphics{bothlinearwcos}}
\caption{\label{fig:epsart}Time evolution of the occupation probability in four-photon KD effect with linear fundamental beam and counter propagating linear third harmonic. The overall laser intensity is $ 3 \times10^{22}$ W$\textnormal{cm}^{-2}$ with wavelength $\lambda=1.03$ nm, field parameters for beam $\omega$ and $3\omega$ are $A_1=18 \times10^{3}$ eV and $A_2=6 \times10^{3}$ eV respectively. The electron enters the laser fields with $p_z=-3k$ along the laser field direction.}
\end{figure}
\begin{figure}[b]

\resizebox{86mm}{68mm}{\includegraphics{bothlinear.eps}}
\caption{\label{fig:epsart} Rabi oscillation in both linear polarization setup for vector potential mentioned in Eq. 10. All other laser and electron parameters are same as Fig. 2.}
\end{figure}
\subsection{\label{sec:level2}Linear Polarization for Two Laser Beams (Lin-Lin)}

In the first setup, the fundamental field and its third harmonic are linearly polarized along the $ x $ axis
 \begin{equation}
\vec{A} =A_1\left[\cos(k(z-ct))\hat{e}_x\right]+A_2\left[\cos (3k(z+ct))\hat{e}_x\right].
\end{equation}
The incident electron is $-3\hbar k$ along the laser propagation direction and has no component parallel to the polarization direction. The overall laser intensity in Lin-Lin setup is $ I=\frac{\omega^2A_1^2+(3\omega)^{2}A_2^2}{8\pi c} $, when the amplitudes of beams are in maximum of their value. The angular momentum of fundamental laser beam $ \omega $ considered for all numerical solutions is $1.2\times10^3 $ eV. Fig. 2 presents the typical behavior of an electron in both linear laser beams. For the electron that is injected with spin up, a Rabi oscillation takes place between $\vert-3,+\uparrow\rangle $ and $\vert+3,+\downarrow\rangle $. The interaction in this field configuration is independent of the initial electron spin state such as the electron in initial momentum and the spin down state $\vert-3,+\downarrow\rangle $ is also scattered into the reflected momentum and spin up state $\vert+3,+\uparrow\rangle $ and the Rabi oscillation is similarly as Fig. 2. This symmetry of spin-flipping exists also in three-photon bichromatic$ (\omega:2\omega) $ KD effect with linear polarization [22].

 The shape of oscillation in bichromatic four-photon KD effect is sinusoidal and has two distinct peaks that are different in size in Fig. 2. It means that the probability of $ \vert c_{-3}^{+\uparrow}\vert^2 $ has sinusoidal oscillation whose minimum amplitude alternatively changes between 0.16 and 0.0 while $ \vert c_{+3}^{+\downarrow}\vert^2 $ oscillate similar to $ \vert c_{-3}^{+\uparrow}\vert^2 $ but it's maximum amplitude changes between 0.84 and 1.0. The Rabi oscillation period is about $ 2.8 $ fs and simulation shows that even with changing the standing waves amplitudes, these two distinct peaks for $ \vert c_{-3}^{+\uparrow}\vert^2 $ and $ \vert c_{+3}^{+\downarrow}\vert^2 $ will not be destroyed.

The vector potential $ A(x)=f(t)[A_1(k_1.x)+A_2(k_2.x)] $ with slow envelope function $f(t)$ which was given in bichromatic $ (\omega:2\omega) $ KD effect demonstrates the typical Rabi oscillation with one peak [22]. Our results confirm that with similar vector potential for bichromatic $ (\omega:3\omega) $ KD effect
\begin{equation}
\vec{A} =f(t)\left( A_1\left[\cos(kz)\hat{e}_x\right]+A_2\left[\cos(3kz)\hat{e}_x\right] \right),
\end{equation}
the typical oscillatory behavior with sinusoidal oscillation appears as shown in Fig. 3. The Rabi cycle is fully developed in Fig. 3 and the period of Rabi oscillation is $ 2\pi/\Omega_R=0.84 $ fs. By comparing vector potentials mentioned in Eq. 9 and Eq. 10, it's obvious that existence of $\cos(\omega_{i=1,2}t)$ part in numerical solutions results in different oscillation behavior.

\subsection{\label{sec:level2}Co-rotating Circular Fundamental and Third Harmonic Fields (Cir-Cir)}
We now look over an electron in two circular bichromatic counter propagating but co-rotating waves given by
\begin{eqnarray}
&\vec{A} =\frac{A_1}{\sqrt{2}}\left[\cos (k(z-ct))\left(\hat{ e}_x+i\hat{e}_y\right)\right]  \nonumber\\
 & +\frac{A_2}{\sqrt{2}}\left[\cos (3k(z+ct))\left(\hat{e}_x+i\hat{e}_y\right)\right].
\end{eqnarray}
If the electron is initially in spin up state with momentum $ -3k $, no diffraction occurs in this field configuration, as shown in upper panel of Fig. 4. In contrast for the electron with spin down and initial momentum $ -3k $ in lower panel, a Rabi oscillation between two states $\vert-3,+\downarrow\rangle $ and $\vert+3,+\uparrow\rangle $ takes place. This spin dependent diffraction behavior implies that it is possible to separate electrons based on their initial spin state in circularly polarized laser beams. The shape of Rabi oscillation in cir-cir setup for an electron with spin down is interesting. Still two peaks in oscillation exist and considering that maximum values of peaks are 1.0 and 0.96, the difference in maximum of peaks is less in this setup. As represented in Fig. 4 for two intervals about $0.56 $ fs the population of modes do not transfer and the electron maintains its momentum and spin. In fact similar to Fig. 2 the electron does not have instant changing momentum and spin. Also in this setup, the vector potential without $\cos(\omega_i t )$ part in Eq. 11 results in the typical sinusoidal Rabi oscillation similar to Fig. 3.

\begin{figure}[t]
 \centering
\resizebox{86mm}{68mm}{\includegraphics{2cir.eps}}
\caption{\label{fig:epsart}Time evolution of the occupation probability in four-photon KD effect with co-rotating circular bichromatic waves. The combined laser intensity is $ 7\times10^{22}$ W$\textnormal{cm}^{-2} $ with wavelength $\lambda=1.03$ nm, field amplitude for both beam is $A_1=A_2=30\times10^{3}$ eV. The electron enters the laser fields with $p_z=-3k$ along the laser direction. Upper panel of the figure shows that electron with spin up does not scatter in this setup.}
\end{figure}

\subsection{\label{sec:level2}Combination of Linear and Circular Polarization Fields (Lin-Cir)}
To examine the result of the last section about spin separation, we focus on a bichromatic setup in which the fundamental beam is linearly polarized and the third harmonic beam is circularly polarized
\begin{eqnarray}
&\vec{A} =A_1\left[\cos (k(z-ct))\left(\hat{ e}_x\right)\right]  \nonumber\\
 & +\frac{A_2}{\sqrt{2}}\left[\cos (3k(z+ct))\left(\hat{e}_x+i\hat{e}_y\right)\right].
\end{eqnarray}
By choosing the high frequency beam to be circularly polarized, as shown in Fig. 5, only the population probability starting from $\vert-3,+\uparrow\rangle $ travels to $\vert+3,+\downarrow\rangle$ state and a Rabi oscillation takes place. The Rabi period is $2.8$ fs and with the same parameters of the lin-lin setup, the population of modes does not transfer completely. The maximum of Rabi amplitude of $\vert+3,+\downarrow\rangle$ state only reaches 0.84.  When the electron spin is down and has $ -3k$ momentum $\vert-3,+\downarrow\rangle $, no scattering occurs at all. According to the $ \textit{S}$ matrix in Eq. 7 by putting $ \epsilon_1=\hat{ e}_x $ and $ \epsilon_2=(\hat{ e}_x+i\hat{ e}_y)/\sqrt{2} $ and due to existence $ \sigma_-$ in Rabi frequency $\hat{\Omega} $, the symmetry transition between the spin up $ \rightarrow $ down and spin down $ \rightarrow $ up disappears.
\begin{figure}[t]
 \centering
\resizebox{86mm}{68mm}{\includegraphics{lincir.eps}}
\caption{\label{fig:epsart}Time evolution of the occupation probability in four-photon KD effect with a hybrid setup that fundamental laser beam linear and the third harmonic is circularly polarized. The other simulation parameters are the same as in Fig. 2. In upper panel electron beam is initially spin up and spin filliping transition occur. The electron beam with spin down in lower panel is not diffracted.}
\end{figure}

 For the case with a fundamental frequency beam of circular polarization and a third harmonic beam of linear polarization, the spin flipping symmetry still exists, i.e. by choosing $ c_{-3}^{+\uparrow}(t=0)=1 $ or $ c_{-3}^{+\downarrow}(t=0)=1 $ the population is transferred to $\vert+3,+\downarrow\rangle $ and $\vert+3,+\uparrow\rangle $, respectively. We have a Rabi oscillation similar to upper panel of Fig. 5 for both electron spin states. In fact, the asymmetry of spin arises only for the circularly polarized high frequency laser beam. As the setup of both linearly polarized beams, if $ cos(\omega_i t)$ is not considered, we find a typical Rabi oscillation.
\subsection{\label{sec:level2} Combination of Linear - Elliptical Polarization Fields (Lin-Ellip)}
When an elliptically polarized laser beam with frequency $ \omega $ and $ \epsilon_1=(2\hat{ e}_x+i\hat{ e}_y)/\sqrt{5}$ is combined with a linearly laser beam of frequency $ 3\omega $ and $\epsilon_2=\hat{ e}_x $, the Rabi oscillation for both up and down spin states of the electron occurs. Numerical results demonstrate well the spin-filliping symmetry. For electron with $ -3k$ momentum, whether the initial spin is up or down, we have a Rabi oscillation behavior as shown in Fig. 6 with dash line. For $ A_1=3A_2=18\times10^3 $ eV the  maximum of Rabi amplitude in this setup is $0.25 $.

 In case of linear polarization for fundamental frequency and elliptical polarization for third harmonic, the vector potential is given by
\begin{eqnarray}
&\vec{A} =A_1\left[\cos (k(z-ct))\left(\hat{ e}_x\right)\right]  \nonumber\\
 & +\frac{A_2}{\sqrt{5}}\left[\cos (3k(z+ct))\left(2\hat{e}_x+i\hat{e}_y\right)\right].
\end{eqnarray}
Solving Dirac equation for this vector potential gives a Rabi oscillation for the electron with initial spin up state as seen in Fig. 6 with solid line. Exactly the same exact Rabi oscillation will be happen if the spin of the initial electron is down. Therefore, with vector potential given by Eq. 13, the diffraction probability dose not depend on the spin orientation of the incident electrons, and with elliptical polarization for high harmonic, unlike circular polarization case, the electron can not be spin polarized.
In fact the Rabi frequency obtained by $ S$ matrix in Eq. 7 also predicst the symmetry of spin-flipping behavior. The inequality of polarization amplitude brings out the existence of $ \sigma_x $ or $ \sigma_y $ in third term of Rabi frequency of Eq. 7. In this condition the separation of electrons due to their initial spin states vanishes.
\begin{figure}[t]
 \centering
\resizebox{86mm}{68mm}{\includegraphics{linellp.eps}}
\caption{\label{fig:epsart}Time evolution of the occupation probability in four-photon KD effect from a linear polarized fundamental laser beam and third harmonic with $ (2\hat{ e}_x+i\hat{ e}_y)/\sqrt{5} $ polarized is shown by solid line. The dash line show the elliptically polarization of fundamental beam and linearly polarization of third harmonic beam. The fundamental laser wavelength $\lambda=1.03$nm and field amplitudes are the same as Fig. 2. For the incident electron with spin up or spin down, the Rabi transitions between two resonant states in any combination of Lin-Ellip configuration will be happen.}
\end{figure}

\section{Conclusion}
Four-photon Kapitza-Dirac scattering occurs in the bichromatic standing wave when the electron beam absorbs three photons from the laser field with $ \omega $ frequency and emits one photon to the counter-propagation laser beam with $ 3\omega $ frequency. The initial electron spin and photon helicity are two factors that can affect on the polarization of the free electron in the bichromatic $(\omega:3\omega)$ KD effect. In this work, it is shown when the fundamental laser beam is linear and 3rd harmonic is circularly polarized, Rabi oscillation occurs only for electrons with spin up. When the initial electrons have spin down, diffraction does not exist and the symmetric flipping spin effect disappears.

In this study, we showed that the shape of Rabi frequency in bichromatic $(\omega:3\omega)$ vector potential has two unequal peaks that change with beam amplitude and the laser intensity. This different oscillation is due to fast time varying $\cos(\omega_i t )$ part in vector potential. Our results also indicate that these two peaks in the Rabi oscillation exist for other harmonics like second and forth harmonics. The Rabi frequency obtained from analytical $\textit{S}$ matrix is congruous with numerical results. Rabi frequency obtained from $\textit{S}$ matrix method predicts that even for other harmonics with circular polarization, the electron is diffracted based on its initial spin state.

The momentum and spin of free electrons in four-photon bichromatic KD effect can be controlled by a suitable laser filed configuration. A spin-unpolarized incident electron beam with $ -3k$ momentum after interaction with a linear fundamental laser beam and third harmonic with circular polarization, splited into two portions $\vert-3,+\uparrow\rangle $ and $\vert+3,+\downarrow\rangle $ with Rabi oscillation. The electron with $+3k$ momentum is entirely spin polarized. By choosing the electron along the laser beams and circular polarization of the high frequency laser beam in bichromatic KD effect, the electron spin filter works for other harmonics participating in the Kapitza-Dirac effect.

\section{References}

redpajama_set_name: RedPajamaArXiv


Stefanie uses breath and awareness in her meditations as a way for teens and adults to find more self-love and kindness in their lives.
Stefanie Goldstein, Ph.D., is a mindfulness teacher, clinical psychologist, and parent to three boys. Her passion is working with adolescents, adults, couples, and families struggling with daily life, helping to support them on their path towards healing and growth. She believes therapy involves all aspects of the self, including the emotional, psychological, physical and spiritual. She specializes in integrating mindfulness when working with stress, anxiety, depression, addiction and trauma. She utilizes an integrative approach by drawing from traditional psychodynamic psychotherapy, mindfulness, cognitive therapy, and somatic psychology. Most importantly, she believes the therapeutic relationship is paramount in the healing and change process. Dr. Goldstein is a trauma specialist and has worked with traumatized teens and their families.


text:
Cecilia Beatriz Buscarons Idoyaga (Juan Lacaze, Uruguay 1949-Barcelona, 2 de julio de 2020), fue una historiadora y escritora uruguaya.

Fue experta en conservación preventiva del patrimonio e investigadora en relaciones de discriminación de género femenino.
Residió en Barcelona desde el 1976, año en el que llegó con su marido y tres hijos emigrando desde Uruguay.

Libros
Escritos por la autora o en autoría compartida:

Artículos

Referencias

Historiadores de Uruguay
Escritoras de Uruguay
Escritores en español
Escritoras feministas de Uruguay
Nacidos en Juan Lacaze
Fallecidos en Barcelona


text:
The numbers show the Green Mile is 5 times harder than the rest of Quail Hollow
Published on Sunday, August 13, 2017
On the scorecard, it doesn't seem too menacing — 1,100 yards, two par-fours broken up by a par-3.
But don't let it fool you, the Green Mile is a beast.
And at the PGA Championship this weekend, the infamous three-hole stretch of Nos. 16, 17, and 18 at Quail Hollow is showing no mercy again.
We took a look at the numbers through the first three rounds to see exactly how painful the final three holes at Quail Hollow have been.
Of the 75 players who survived the cut, only five played the Green Mile under par through Round 2. Seven have played it even, while 63 have been over.
The average score on the par-11 Green Mile was 11.76. Per hole, that's 0.25 strokes more than par for each, roughly five times harder than the other 15 holes are playing.
Among the 75 golfers still playing, there were no eagles, 57 birdies, 435 pars, 145 bogeys, 33 doubles, four triple bogeys, and one quadruple on the stretch through three rounds.
And of the three Green Mile holes, the par-4 18th has proven to be the hardest. The 75 players left combined to shoot 70-over on the final hole, an average of 0.31 strokes over par per player. The 18th has seen 12 double bogeys, a triple, and a quadruple among the 75 players left.
Hole 16 Hole 17 Hole 18
Birdies 17 22 18
Pars 150 149 136
Bogeys 47 41 57
Doubles 10 11 12
Triples 1 2 1
Quadruples 0 0 1
TOTAL SCORE +53 +36 +70
But there are some outliers:
Ryan Fox — who finished Saturday at 1-under, tied for 12th place — shot a combined 2-under on the Green Mile in his first three rounds. Fox birdied 16 in his first two rounds and shot par on 17 and 18 in all three.
On the other end of the spectrum is Russell Henley, who is 9-over on the Green Mile through three rounds. Henley carded a double-bogey on 17, then a bogey on 18 in his first round, bogeyed 16 and 18 in Round 2, and bogey 16, then triple-bogeyed 18 in his third round.
The 54-hole leader, Kevin Kisner, ended his third round at an impressive 7-under, and a large part of that may be due to his performance on the final three holes of the course — an even par.
The lesson? When it comes to the Green Mile, there is but one mantra worth following: Survive.


It doesn't happen often that I am jealous of people working for an institution, but for the splendid web team of the European Parliament I am glad to make an exception. Find out why in their extremely well-done and entertaining video – 5 minutes and 5 seconds of your time that won't be wasted. (Video afte There is a little more context on their team blog.
Writing for (y)EU – Full edit from Web Com on Vimeo.
Thanks for your support! we're happy you like it.
Pleasure! Thanks to you and the team for doing such splendid work in an usually-difficult environment – and sharing the fun parts of it!
Difficult environment? Where? Who. What makes you say that. Ah und so, neidisch bist? Ich interpretiere das jetzt mal ganz unzweideutig.


Make sure that your browser is set to accept cookies. This is what enables the Night Sky Network website to identify you as you click from page to page after logging in.
Chrome: From the "Customize and Control Chrome" menu at the top right (which sometimes appears as three vertical dots), choose "Settings". Click "Show Advanced Settings" at the bottom of the page. Under Privacy, click the "Content Settings" button. Make sure "Allow local data to be set" is checked under "Cookies".
For more information, see Google's help page on this topic.
Firefox: Click "Open Menu" (the three horizontal bars at the top right). Select "Options", and then click the "Privacy" option on the left. You can check the options in this menu to make sure cookies are not disabled or blocked for nightsky.jpl.nasa.gov.
For more information, see Mozilla's help page on this topic.
Internet Explorer: From the "Tools" menu (the gear at the top right), select "Internet Options", and then click the "Privacy" tab. Set your Privacy level to "Medium" if it is set any higher. If you still wish to disable cookies on websites other than the Night Sky Network, click "Sites" and enter http://nightsky.jpl.nasa.gov as one of your allowed websites.
For more information, see Microsoft's help page on this topic.
Safari: Choose "Preferences" in the Safari menu. Click "Security". Under "Cookies and website data", choose "Allow from websites I visit".
For more information, see Apple's help page on this topic.
Others: Consult your browser's Help option for instructions on how to enable cookies.
Clear your browser's cache, and make sure that your browser is set to check for a new version of each page you visit upon every visit, rather than storing pages for later re-use. This will also ensure that you are seeing the latest updates on the Night Sky Network home page.
If you are still having difficulties, you may contact the Night Sky Network's administrators. Just fill out the form below with your Username (if you know it), real name, club name (if you belong to a club), email address, and a message describing your problem.


Lovely turnkey home in a quiet neighborhood in Corona. 3 BR + 2.5 BA with 1,690 sf living space on 6,534 sf lot, and permitted addition of 308 sf covered patio with 224 sf patio enclosure (copy of permit attached with property photos). Features and upgrades: cathedral ceilings; wood & tile flooring; fireplace in family room; kitchen with built-in stainless steel appliances, recessed lights, eating area and walk-in pantry; separate laundry area; master bedroom with walk-in closet; master bathroom with separate tub and shower; covered patio with enclosed sunroom/exercise room and many more. A must see!


text:
STORY FROM THE FIELD – Rouamba Odile
by The Sonder Project | Mar 14, 2019 | Burkina Faso, Farms, Global Projects
Rouamba Odile is a fighter. She was born in the 1960's in Burkina Faso, but she's not sure exactly when. She never went to school and she isn't able to read/write. Her father tried to arrange her marriage at the age of 17, but she ran away to her sisters house in a nearby city. Her father tried to take her back, but instead she ran away again with her current husband to the Ivory Coast. She had 8 kids, although she lost 1 adult child.
Twenty years later, she was able to reconcile with her family, and she returned with her family to Burkina Faso. She gained a reputation for being a peacemaker and describes herself as the village grandmother, but she never had an opportunity to really lead, always playing the second fiddle to her husband. Althought when it came time for her community of Komsnedego to select a female village leader for The Sonder Project Community Farm, Rouamba was chosen for her ability to work with others.
Thanks to the Community Farm, Rouamba said her family will no longer face food insecurity, and they will now have a year-round opportunity to generate income. She also believes the Farm may help draw back two of her children who still reside in the Ivory Coast. She never thought the community would have such an opportunity, it's a dream come true.
photography: Tara Rice


text:
Report: Wojciech Szczesny to Juventus is a done deal
By Danny Penza@djp4cal Updated Jun 6, 2017, 2:05am CEST
Share All sharing options for: Report: Wojciech Szczesny to Juventus is a done deal
Photo by Emilio Andreoli/Getty Images
When reports first surfaced that Juventus were targeting Wojciech Szczesny and that the Polish goalkeeper could very well end up being the summer's first official acquisition, I was one to think to myself, "Ha ha, okay, very funny, guys." It was the night before the Champions League final. I was in no mood to hear about it. I had more important things to worry about — and that was before Juve laid an egg in the second half against Real Madrid.
And yet, as we sit here three days after the initial reports came about, they aren't going away.
They're getting even stronger.
Sky Sport Italia transfer master Gianluca Di Marzio is reporting that Juventus have discussed things with Arsenal and the two clubs have agreed to a fee Szczesny, who spent the last two seasons on loan at Roma. This comes after reports surfaced over the weekend that Szczesny and Juventus had agree to personal terms on a four-year contract. Put two and two together and you have, at least when it comes to what the media is reporting, a deal that looks like it will be happening.
More from Di Marzio:
About the goalkeeper, the deal for Szczesny is wrapped up. Arsenal and Juventus have agreed on a 14 million euros deal with 2 more million bonus. The player will get a four year contract with four million euros per season, with a last year augmentation about 4.5 million euros.
Now we wait and see if all of this comes to fruition.
There are obviously two big dominoes that comes with this:
Juventus' backup keeper for the last two seasons, Neto, will probably be leaving if Szczesny does indeed sign with the six-time defending Serie A champions in relatively short order.
Juventus may as well deem Szczesny the replacement for Gigi Buffon when he retires.
Basically, you don't sign a goalkeeper for that kind of money if you don't view him as a starter at least some time down the road. Rarely do teams spent huge amounts of money for their starting goalkeeper — look at how long Buffon's transfer fee from Parma to Juventus has been the world record — and even less for the No. 2. But potentially €16 million for somebody who will deputize for Buffon next season? Yeah, there's something going on more than just trying to upgrade your backup goalkeeper.
I guess it might be time to learn how to spell "Szczesny" without using copy/paste, folks.