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Something we've known for a long time has just been publicly acknowledged by Seattle Business Magazine: Legacy is one of the Top 100 Places to Work in Washington!! Founded on solid values, guided by excellent leadership, and made up of high quality humans – it's a great place to be.
Legacy provides essential services to the wireless industry from the Pacific Northwest to the Great Plains.
We build and maintain the structures and systems that keep you connected!
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I just wanted to take a moment between fire drills and let you know your Project Manager has been a tremendous help with the……tower project. His patience and professionalism is very much appreciated. His ability to comprehend, organize, schedule and keep the ball rolling is going to make this project a success. Thank you!
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Mrs. Bork was awarded a grant from The McLoud School Foundation for student notebooks, scissors, glue, colored pencils, sharpeners, and other supplies that her students use on a daily basis. MJH is extremely grateful for this generous funding opportunity.
Representing McLoud!
ECC teachers Loud and Proud for McLoud!!
Walkout Revised- PLEASE READ
Walkout Update
McLoud Juniors will be taking the ACT tomorrow, April 3rd. Please be to school on time and ready to take the test. You will need to go to the High School West building.
McLoud Public School will resume school Tuesday, April 3rd.
CONGRATULATIONS 🍾🎊🎈 The McLoud Schools Foundation presented grants totaling $2,791.35 to four second and third grade McLoud Elementary teachers today. Thank you for your support of our kids! We appreciate you! Mrs. Nikkel and Mrs. Stotts (on each end) of the foundation are pictured with teachers, April Mooney, Beth Bruns, Elsie Little, and Linda Ogle. Also, Ms. Meese, who is pictured with the Intermediate teamed up with the ladies on their projects!
The McLoud Schools Foundation presented grants totaling $6,286.74 to seven teachers at the ECC today. We appreciate their support of our teachers and students so much!! Mrs. Stotts and Mrs. Nikkel of the foundation are pictured with the teachers: Amy Young, Leslie Lane Norwood, Mindy Love Smith, Felicia Hayes, Chrisanna Collinsworth Looney, Kami Baker, and Kena Utter.
McLoud high school baseball tournament scheduled for Thursday, March 29 has been canceled. A revised schedule will be posted later today.
Students that got all A's, no more than 2 tardies, and no unexcused absences got to go on a rewards trip to a trampoline park today. Good job students keep it up!
Sack lunches will be provided at the ECC Monday, April 2 for any McLoud Student wishing to get one. Hours will be from 11:00 am-1:00 pm. This service will continue as needed if a school stoppage occurs.
McLoud High School Juniors will be taking the ACT Test on Tuesday, April 3, 2018 even if a school stoppage occurs. Please be at school no later than 8 a.m. If you need transportation please call the High School. Breakfast and lunch will be provided.
Parent Information: School Stoppage
JH & HS baseball and soccer are cancelled today due to rain.
McLoud Jr. High wants to congratulate Leslie Bork for being selected as our Teacher of the Year! She is creative, hard-working and caring! She has what it takes to teach 8th grade Social Studies. Awesome job Mrs. Bork!
Show your support for public education this week!
Faculty vs Student basketball 2018
ECC students learned dental hygiene from Captain Supertooth today!
McLoud Public Schools

subset: commoncrawl


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Listening to the Dharma is the beginning of all...
Viriyalila, FBA Team
Kalyanavaca, London, UK
Kuladharini, Glasgow, UK
Mary, FBA Team
Sanghajivini, Newcastle, UK
Vajratara, Sheffield, UK
Buddhasiha, Ipswich, UK
Advayasiddhi, Denmark
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Please visit one of the talks pages and select (See All) from one of the talks panels.
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text: Victorinox Swiss Army Knife Champ Top 10 Swiss Army Knives 14 September, 2011 Swiss army knife is one of the coolest gadgets and an easily recognizable brand around the world. Swiss army knives from Victorinox and Wenger are pretty useful tools that fit neatly into your pocket. Today, we have a list of some of the best Swiss army knives around. No 10. Sigg Folding Clip Cutlery Set Read More Amazing Floppy Disk Art Anonyzious Pegasus Sculpture Made From 3500 Phones Anonyzious Incredible Everyday Gadgets You Want To Have Anonyzious The Difference Between Europe & America Anonyzious Enabling FaceTime on iPhone 3GS Anonyzious Top 10 Mega Machines Anonyzious Be Amazed At This Artist's Unique Psychedelic Art Creations Anonyzious Without updating 3.1 enable MMS on iPhone 3.0 Anonyzious LG Introduces World's Slimmest Full HD Panel Anonyzious You are not hallucinating – this car runs upside down Anonyzious


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- How much does social security charge for name change?
- How do I find my legal name?
- Why did immigrants change their names?
- Can I keep my maiden name on my Social Security card?
- What is previous legal name?
- How long does it take for your name to change?
- Can I change my name for free?
- How do I change my first and last name?
- How do you write a letter to request a name change?
- How do I trace a name change?
- How difficult is it to change your name?
- Do you get a new credit file when you change your name?
- What is it called when you change your name?
- Who do you need to tell when you change your name?
- Will changing my name give me a new credit file?
- What is considered a legal name change document?
- What is considered your full legal name?
- How do I find someone if I only know their maiden name?
- What do you bring to change your name?
- Can I be tracked if I change my name?
- How do I fill out a name change form?
How much does social security charge for name change?
If you legally change your name because of marriage, divorce, court order or any other reason, you must tell Social Security so you can get a corrected card.
You cannot apply for a card online.
There is no charge for a Social Security card.
This service is free..
How do I find my legal name?
The "legal name" of an individual usually consists of a given name, usually assumed at birth and a surname deriving from the common name of your parents unless you become married when you may choose to use your spouse's surname.
Why did immigrants change their names?
More commonly, immigrants would change their names themselves when they had arrived in the United States, and for a number of reasons. … Someone might change their name in order to make it sound more American, to fit in with the local community, or simply because it was good for business.
Can I keep my maiden name on my Social Security card?
If your decree or dissolution specifies a new name, the SSA must use it. If it's omitted, you can revert to any prior name they have on file. Returning to a name that's not on file requires proof, such as a birth certificate for maiden name or marriage certificate for a prior married name.
What is previous legal name?
Former name refers to any surname (last name) you may have used in the past for any reason. It can also mean any first and last name you may have used in the past. … Former name is Jones, your surname before you got married.
How long does it take for your name to change?
Name change actions can take anywhere from a day, to six (6) months (sometimes even longer). The time it takes for name change actions to be ordered/decreed varies not only from state to state but from county to county and courthouse to courthouse as well.
Can I change my name for free?
The Social Security Administration has its own form which you can get for free. The good folks at SSI will also let the IRS know about the name change, so you're good to go. When you go to the DMV, you'll just need to bring the certified copy of the marriage certificate and you'll be done.
How do I change my first and last name?
The process to legally change your name is the same whether you want to change your first or last name. Although the steps vary by state, almost every state requires you to file a petition with the county court where you live, seeking the court's permission for your proposed change.
How do you write a letter to request a name change?
This letter is to inform you officially that I have legally changed my name. My previous name that is currently on file in the bank for the above account is PREVIOUS NAME. I request you to change your records to my legal name: NEW LEGAL NAME. I have enclosed a copy of proof of my name change.
How do I trace a name change?
How to Find Out If Someone Legally Changed Her NameDo some internet research. As a preliminary step, search the web and social media for the individual you are seeking. … Check with the county courthouse. An individual can easily change their name because of marriage, divorce, or any other reason, as long as it's not unlawful for fraudulent.
How difficult is it to change your name?
Although it may be seem daunting to show up at court or fill out legal paperwork, you don't need to hire a lawyer to change your name. Filling out a Petition for Name Change can be fairly straightforward. But if you do feel overwhelmed by navigating the name change process yourself, consider outside help.
Do you get a new credit file when you change your name?
Does a new name mean you get a new credit score? Unfortunately for anyone who's hoping for a do-over, changing your name doesn't reset a poor credit score or wipe out your existing credit report to let you start anew. Your new name simply gets added to your existing credit report.
What is it called when you change your name?
Name change generally refers to the legal act by a person of adopting a new name different from their current name. … Pseudonyms are generally adopted to conceal a person's identity, but may also be used for personal, social or ideological reasons.
Who do you need to tell when you change your name?
Nina Callaway is a longtime freelance writer with over 15 years of experience….Government AgenciesSocial Security Administration. This is where you get a new social security card.Department of Motor Vehicles. … Voter Registration. … State Department.
Will changing my name give me a new credit file?
No — not if you tell all record holders about your new name. … The credit reference agencies can correlate your credit history from your old and new names. However, you should make sure that you tell all financial organisations — banks, credit card companies, lenders, etc. — about your change of name.
What is considered a legal name change document?
With a court order you can change your legal name on government-issued identification documents such as your driver's license, passport, and social security card. You will generally need a certified copy of the decree changing your name.
What is considered your full legal name?
Definition of Full legal name Full legal name means the applicant's first name, middle name(s), and last name, without the use of initials or nicknames, as it appears on the applicant's presented source documents.
How do I find someone if I only know their maiden name?
The best place to locate a woman's maiden name is on a marriage record (both civil and religious). These records include licenses, banns, bonds and consent affidavits. A Bann is an announcement of an intended marriage usually made in church on three successive Sundays.
What do you bring to change your name?
You will also need to bring the following documents:Proof of Citizenship: your valid passport or a certified copy of your birth certificate.Proof of Name Change: a certified copy of your marriage license. … Proof of Identity: This must show your name, date of birth or age, and have a recent photograph.More items…•
Can I be tracked if I change my name?
Yes you can be traced if you change it by deed poll. All deed polls are published in The Gazette, an arcane publication of official 'stuff' this is then used by various govt and private organisations to update their records. It is a public document. But most lay people would not know how to go about doing this.
How do I fill out a name change form?
You can obtain a Name Change Petition from your local Clerk of Court.Write down your current name as the petitioner. … Write down your current name again. … Write down your address and place of birth. … Confirm that you have never been convicted as a sex offender. … Explain the reason for the name change.


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Date of publication: 2020-08-20 07:02
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Am I wrong for feeling this way?
So I'm currently visiting my bfs family and we've been them visiting for about a month or so now. We're staying in a two bedroom house that has 7 kids and then his cousin and her husband (4 kids are theirs) and his aunt and his other cousin live in the other bedroom (other 2 is his aunts and 1 is the cousins). Well first let me tell ya'll that it gets super hot and humid in this house.. there's a baby almost 5 months upstairs so they don't allow us to turn on the air conditioning so we've been using a fan from the very beginning.. well his cousin and her husband took the fan upstairs so we've been burning up all night. They live in gated apartments and so we've been opening the door a little btw were all the way downstairs for maybe about an hour or two at a time.. and his aunt walked down and got mad at us for having it open so we turned on the air for maybe 10 min (THATS HOW HOT IT WAS.. WE WERE SWEATING) if even that and they got mad at us again and then the next day the baby was sneezing so they blamed us for the air on (we didn't know at the time they didn't want it on) but the only thing i can think of is the fan they use because it has loads of dust built up in it.
So another incident we had.. we bought our own food and a shitload of it (they don't share theirs) which i have no problem doing.. I got it Saturday and by Monday majority of it was gone because they just let their kids eat it after we made it clear it was ours so that was kind of annoying too.
Then we ran out of food and we were ordering a pizza. We even waited until the kids were at practice and got it but my bf's cousins husband came home. Later that night my bf's cousin (the wife) calls him upstairs and asked him why we didn't buy 3 or 4 pizzas for everyone? Basically making a huge deal that we didn't offer any and that we should have bought everyone some which is bullshit because we specifically waited until all the kids were gone.
NOT TO MENTION WE CAME HERE NOT AWARE THAT THERE IS COCK ROACHES. Nobody even told us. There are seriously loads of them and they have to sleep with the lights on. I'm not trying to be ungrateful or anything but how they've been setting rules on us is really irritating. Their kids are little monsters and are so disrespectful. I'm going crazy. We only have 2 days left THANK GOD.
UPDATE: Um all of you are saying "why are you visiting so long" "there annoyed" but first off they asked us to come stay with them so we don't waste a lot of money and it's a long ways from home and they wanted us to stay this long. We've been planning to come for the longest time now. Also one of my bf's grandpa has cancer and that's why we planned on coming and staying because he's on his death bed.


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So here we are on a rather grey, windy and rainy Monday, and time to recall the small pleasures of the week and ignore the weather outside. First up, of course, we have to mention Jacinda Ardern being elected for a second term.
Tag: Arobake
This week's small pleasures #212
So….here we are…another Monday…..and the skies are grey and the rain is pouring down in contrast to weather earlier last … More
This week's small pleasures #192
Since last week's small pleasures post I have gone shopping, eaten out and bought flowers. I know. 6 weeks ago … More
This week's small pleasures #186
So here we are again with another round of lockdown small pleasures. These can be as simple as a fun … More
If we were having coffee…or even a cup of tea…
If we were having coffee…or even a cup of tea…we would, of course, be doing so from our own homes … More


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- Is calculus more difficult than trigonometry?
- Is Trig easier than pre calc?
- Should I take calculus or trigonometry?
- Why is calculus so hard?
- Is calculus the same as trigonometry?
- Which calculus is the hardest?
- What is the hardest type of math?
- Can I take calculus without trigonometry?
- Does trigonometry prepare you for calculus?
- Is Precalc harder than algebra 2?
- Is calculus really that hard?
- Is physics harder than calculus?
- Which comes first calculus or trigonometry?
- What math comes after trigonometry?
Is calculus more difficult than trigonometry?
Calculus is probably more difficult because it is less in accordance with our everyday experiences.
It is also a much more varied topic and more powerful.
Of course one can always find harder and harder problems in either topic but calculus includes much trig..
Is Trig easier than pre calc?
Precalculus, which is a combination of trigonometry and math analysis, bridges the gap to calculus, but it can feel like a potpourri of concepts at times. … Now, most students agree that math analysis is "easier" than trigonometry, simply because it's familiar (i.e., it's very similar to algebra).
Should I take calculus or trigonometry?
If they have, you probably don't want to skip Pre-Calculus. … On the other hand, you must have a strong background in Algebra, and Trigonometry to understand Calculus. Do not, under any circumstances, consider skipping Trigonometry before taking Calculus.
Why is calculus so hard?
When students find calculus difficult, it is often because of a failure to recall important concepts they learned in algebra, geometry, and precalculus{usually third level algebra combined with elementary functions and trig}.
Is calculus the same as trigonometry?
Calculus is the study of differentiation and integration. Trigonometry is the study of triangles.
Which calculus is the hardest?
Calculus 3In a poll of 140 past and present calculus students, the overwhelming consensus (72% of pollers) is that Calculus 3 is indeed the hardest Calculus class.
What is the hardest type of math?
So, here are top 10 most tough topics of mathematics that usually students struggle with:Algebra: … Calculus: … Geometry and topology: … Combinatory: … Logic: … Number Theory: … Dynamical Systems & Differential Equations: … Mathematical Physics:More items…•
Can I take calculus without trigonometry?
Yes, but can you take pre calc without having taken trig. At the high school level, yes, although exposure to basic right triangle trig in a geometry or algebra 2 class would help. If a high school offers precalculus, then they normally do not offer a separate trig course, but there are exceptions.
Does trigonometry prepare you for calculus?
Otherwise, yes, trigonometry plays a pretty big role in the methods, if not the theory, of the Calculus, and is definitely a prerequisite (but it is also very important in physics and engineering, so Calculus is not the only place you'll use it if you're going into a field in which those are requirements).
Is Precalc harder than algebra 2?
Precalculus is fundamentally harder than Algebra II since it incorporates all the concepts previously learned in Algebra, Geometry, and Algebra II as well as including new, more challenging material. The second semester was completely covered and re-taught in the first semester of Precalculus.
Is calculus really that hard?
Calculus is a very difficult subject and one that a lot of students have trouble with. Calculus is a very difficult subject and one that a lot of students have trouble with. Indeed, it is the toughest course at YSU. If it is any consolation, you should remember that, generally, only strong math students take Calculus.
Is physics harder than calculus?
Hands down, physics is harder than calculus. The reason is simple, for physics, you need to have rigorous understanding in both physics concepts and calculus itself. Meanwhile, if you learn calculus, you might (only) need to master the concept of calculus.
Which comes first calculus or trigonometry?
Trigonometry should be taken before calculus.
What math comes after trigonometry?
Advanced Algebra / Trig Immediately follows Algebra II. Covers all of Trigonometry and some of the Math Analysis SOLS. Counts toward an Advanced Diploma. This class provides a good foundation for students going on to community college or a four year college.


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Fans who have had to make do with months of television repeats can now look forward to the real thing again, with England captain Joe Root saying of the West Indies' decision to tour: "It must be extremely scary and I think the whole cricketing world will be grateful to see some cricket again."
The three-match contest was originally meant to be played in June but will now start on July 8 instead because of the COVID-19 pandemic.
"This is a huge step forward in cricket and in sports in general as we travel over to England for this series," said Holder.
"A lot has gone into the preparations for what will be a new phase in the game."
Welcome to England @windiescricket! 👋We are delighted to have you here and can't wait for our Test series to get… https://t.co/eZb0JIOrZH
— England Cricket (@englandcricket) 1591695238000
But rather than matches before crowds at The Oval, Edgbaston and Lord's, a now back-to-back series will take place behind closed doors at the more 'bio-secure' Ageas Bowl and Old Trafford.
Whereas players usually spend evenings during a Test away from the ground, they will now instead find themselves in a protective bubble at two venues which both have onsite hotels.
Southampton's Ageas Bowl will stage the series opener from July 8, with the next two Tests at Old Trafford.
All the West Indies players have tested negative for the virus, although they will be retested when they arrive in Manchester.
Health measures, including a ban on applying saliva to the ball set to be rubber-stamped at an International Cricket Council meeting on Wednesday, will be in place.
"Our main objective is to deliver a safe environment for all stakeholders," said England and Wales Cricket Board events director Steve Elworthy.
Yet there is no escaping the financial impact of the virus.
Going ahead with major matches is seen as vital, with the ECB estimating it could lose £252 million ($316 million) if there are no fixtures at all this summer.
One of cricket's poorest major teams in the West Indies is now helping one of its wealthiest, despite the Caribbean outfit's cricket board having to impose a 50-percent pay cut on all players and staff.
The West Indies, who hold the Wisden Trophy after beating England at home last year, have selected a 25-strong squad.
They will complete a 14-day quarantine period combined with initial training at Old Trafford before heading south from Manchester for the first Test.
Despite the ECB's efforts, three West Indies players — Darren Bravo, Shimron Hetmyer and Keemo Paul — declined to tour, with Cricket West Indies insisting it will not hold this against them when it comes to future selection.
Bravo and Hetmyer's absence deprives the tourists of two top-order batsman, with Paul less of a loss given he is a back-up for Holder, the world's top-ranked allrounder.
Former interim head coach Floyd Reifer will fill in as batting coach for Monty Desai, who is based in India and cannot join the tour due to travel restrictions.
"There is expectation in the air that we will defend the Wisden Trophy and we will certainly put in the work and give it our all to keep hold of it," insisted Holder.
But it could be Root who is the most significant absentee from the first Test.
Root's wife is expected to give birth to the couple's second child in the first week of July.
That may mean Root has to then self-isolate for seven days, putting a question mark against his participation at Southampton.
Root has backed vice-captain Ben Stokes to do a good job in his absence but Kevin Pietersen, recalling his own brief stint as England skipper, was wary of adding to the star all-rounder's burdens and suggested wicketkeeper Jos Buttler for the role instead.
"The entertainers and the guys that have to carry the mantle in the team sometimes aren't the best captains and sometimes struggle with the extra added pressure," Pietersen told talkSPORT.


text:
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The initial dose is 4 mg with titration to 4 mg three times a day.
© Copyright 2017-2019 - EridanusPills. All rights reserved. Site Map


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In 2006, a group of thieves performed what is considered one of the most famous and smart bank heists in the history of Argentina. How they robbed the Rio bank is as surprising as what happened afterwards. This is their story.
Heidi, bienvenida a casa
Centered around 3 couples lives in Argentina as they deal with life, personal problems, and each other. Three boys work in the same office and each of their girlfriends end up becoming friends. Lies and drama build up and tie all of their lives together in a way.


text:
production and limits on anomalous and couplings in collisions at TeV
We present a measurement of (, ) production with a data sample corresponding to an integrated luminosity of 6.2 fb collected by the D0 detector at the Fermilab Tevatron Collider. The results of the electron and muon channels are combined, and we measure the total production cross section and the differential cross section , where is the momentum of the photon in the plane transverse to the beamline. The results obtained are consistent with the standard model predictions from next-to-leading order calculations. We use the transverse momentum spectrum of the photon to place limits on anomalous and couplings.
pacs:12.60.Cn, 13.85.Rm, 13.85.Qk
The D0 Collaboration111with visitors from Augustana College, Sioux Falls, SD, USA, The University of Liverpool, Liverpool, UK, UPIITA-IPN, Mexico City, Mexico, SLAC, Menlo Park, CA, USA, University College London, London, UK, Centro de Investigacion en Computacion - IPN, Mexico City, Mexico, ECFM, Universidad Autonoma de Sinaloa, Culiacán, Mexico, and Universität Bern, Bern, Switzerland. Deceased.
I Introduction
The standard model (SM) describes the electroweak interactions through a non-abelian gauge group , which includes self-interactions of gauge bosons. Because the boson carries no electric charge, a coupling between a boson and a photon is not permitted. The production in the SM is dominated by the lowest-order Feynman diagrams shown in Fig. 1.
An excess in the number of high-energy photons can be a sign of new physics, e.g., supersymmetry, as described in Ref. zgammaSUSY or new heavy fermions with nonstandard couplings to the gauge bosons, as discussed in Ref. zgammaSUSY2 . Such an excess of high-energy photons can be described by assuming only Lorentz and local gauge invariant and trilinear gauge boson vertices of the form shown in Fig. 2, using an effective theory with eight complex coupling parameters, , where = and or hzp . Here, the couplings parameters and ( and ) are associated with dimension-six (dimension-eight) operators which allow for an interaction between a boson and a photon. To conserve tree-level unitarity at asymptotically high energies, one can introduce form factors dependent on the square of the partonic center-of-mass energy, , given by , where is the mass scale at which the new physics responsible for anomalous couplings is introduced baur . These anomalous gauge boson couplings would give rise to an excess of photons at high transverse momentum, , which can be searched for by measuring the total production cross section and the differential cross section for ( henceforth) production. If no evidence of new physics is seen, we can place limits on the real components of the -even coupling parameters, and , for and TeV. Following Ref. baur , we choose form-factor powers for the unitarity scaling dimensions of for and for . production has been previously studied at collider experiments zgammaprev8 ; d0prev ; zgammaprev5 ; zgammaprev2 ; zgammaprev7 ; zgammaprev6 ; zgammaprev4 ; zgammaprev3 ; zgammaprev1 , and because the value of greatly affects the scale of anomalous production, we choose to perform this analysis for the values of that were used by the recent D0 zgammaprev8 ; d0prev and CDF zgammaprev5 analyses. This choice of differs from the value used by the ALEPH zgammaprev2 , CMS zgammaprev6 , DELPHI zgammaprev4 , L3 zgammaprev3 , and OPAL zgammaprev1 collaborations.
We present measurements of the inclusive cross section and differential cross section for production in the electron and muon channels using a data sample corresponding to an integrated luminosity of 6.2 0.4 fb collected at TeV by the D0 detector at the Fermilab Tevatron Collider between June 2006 and July 2010. These results provide a significant improvement in the sensitivity to anomalous and production compared to a previous D0 publication, utilizing the same channels and an integrated luminosity of 1 fb zgammaprev8 . In addition to increasing the size of the data set, we also combine with a previous result in the same channels zgammaprev8 , along with another D0 result d0prev that used 3.6 fb of production to place stringent limits on anomalous couplings.
Ii The D0 Detector
The D0 detector dzero1 ; dzero2 ; dzero3 ; dzero4 ; dzero5 consists of a central tracking system contained within a 2 T superconducting solenoidal magnet, surrounded by a central preshower (CPS) detector, a liquid-argon sampling calorimeter, and an outer muon system. The tracking system, consisting of a silicon microstrip tracker (SMT) and a scintillating fiber tracker (CFT), provides coverage for charged particles in the pseudorapidity range d0_coordinate . The CPS is located immediately before the inner layer of the calorimeter and has about one radiation length of absorber followed by several layers of scintillating strips. The calorimeter consists of a central cryostat sector (CC) with coverage and two end calorimeters (EC) which extend coverage to . The electromagnetic (EM) section of the calorimeter is segmented into four longitudinal layers (EM, ) with transverse segmentation of , except in EM3, where it is . The muon system resides beyond the calorimeter and consists of a layer of tracking detectors and scintillation trigger counters before a 1.8 T iron toroidal magnet, followed by two similar layers after the toroid. The coverage of the muon system corresponds to a pseudorapidity range .
Iii Event selection
Candidate events are selected in the and ( and henceforth) final states. The interaction vertex must be reconstructed within cm of the center of the D0 detector along the beam () axis. For the electron channel, a sample of candidate -boson events is collected with a suite of single-electron triggers. The electrons are selected by requiring an EM cluster in either the CC () or EC () regions of the EM calorimeter with transverse momentum (15) GeV/ for the electron candidate with the highest (next-to-highest) transverse energy contained within a cone of radius , centered on the axis of the EM shower. At least 90% of the cluster energy must be deposited within the EM section of the calorimeter. Electron candidates, with a shower shape consistent with that of an electron, are required to be spatially matched to a track and to be isolated in both the calorimeter and tracking detectors. To suppress jets and photons misidentified as electrons, a likelihood discriminant is built using a set of variables sensitive to differences in tracker activity and energy deposits in the calorimeter: the number of tracks and the scalar sum of the transverse momentum of all tracks within of the EM cluster, the fraction of energy deposited in the EM section of the calorimeter, the longitudinal and transverse shower profile in the calorimeter, and the ratio between the transverse energy in the calorimeter and the transverse momentum of the electron associated track. To further suppress jets misidentified as electrons, in particular, for high instantaneous luminosity conditions, a neural network algorithm is trained on Drell-Yan and jet data, using information from the calorimeter and CPS: the numbers of cells above a threshold in EM1 within 0.2 and 0.2 0.4 of the EM cluster, the number of CPS clusters within 0.1 of the EM cluster, and the squared-energy weighted width of the energy deposit in the CPS. Events where both electrons are contained within the EC are excluded because of the small signal acceptance. Candidate events where the boson decays into two muons are collected using a suite of single-muon triggers. Within the muon channel, muon candidates are required to be within and matched to a well-isolated track in both the tracker and the calorimeter with transverse momentum GeV/. The highest muon must have 20 GeV/. Both muon candidates are required to originate from within 2 cm of the interaction point in the direction.
Photon candidates in both the electron and muon channels are required to have transverse momentum GeV/ within a cone of radius centered around the EM shower in the CC. The rapidity of the photon, , is required to be . Additionally, the photon candidate must satisfy the following requirements: (i) at least of the cluster energy is deposited in the EM calorimeter; (ii) the calorimeter isolation variable 0.15, where is the total energy in a cone of radius and is the EM energy in a cone of radius ; (iii) the energy-weighted cluster width in the EM3 layer is consistent with that for an EM shower; (iv) the scalar sum of the of all tracks, , originating from the interaction point in an annulus of around the cluster is less than 2.0 GeV/; (v) the EM cluster must not be spatially matched to either a reconstructed track or to energy depositions in the SMT or CFT detectors that are compatible with a trajectory of an electron HOR ; and (vi) an output larger than 0.1 of an artificial neural network () ANN5 that combines information from a set of variables sensitive to differences between photons and jets in the tracking detector, the calorimeter, and the CPS detector.
The dilepton invariant mass, , is required to be greater than 60 GeV/, and the photon must be separated from each lepton by . Additionally, each lepton must be separated from a jet by . In the electron and muon channels, we select 1002 and 1000 data events, respectively. In order to reduce the contribution of final-state radiation (FSR), subset data samples are defined with the requirement that the reconstructed three-body invariant mass, , exceeds 110 GeV/. With this additional requirement, 304 and 308 data events are selected in the electron and muon channels, respectively.
iii.1 Background subtraction
The selected sample is contaminated by a small admixture of jet events in which a jet is misidentified as a photon. To estimate this background in the electron channel, the fraction of jets that pass the photon selection criteria but fail either the or the shower width requirement, as determined by using a dijet data sample, is parametrized as a function of and (ratio method). The background from +jet production is then estimated starting from a data sample obtained by reversing the requirements either on or on the shower width requirement, and applying the same parametrization. A systematic uncertainty associated with the estimation of the number of real photons in the data samples is due to the finite size of the dijet background sample. After subtracting the estimated background from the data in the electron channel, we estimate 926 53 (stat.) 19 (syst.) signal events when no requirement is applied, and 255 15 (stat.) 5 (syst.) signal events with GeV/.
To estimate the background in the muon channel, we use a matrix method to estimate the +jet background contribution. After applying all of the selection criteria described above, a tighter requirement on is used to classify the data events into two categories, depending on whether the photon candidate passes () or fails () this requirement. The corresponding number of events compose a 2-component vector (, ). Thus, the sample composition is obtained by resolving a linear system of equations , where () is the true number of (jet) events in the fiducial region. The efficiency matrix contains the photon and jet efficiencies that are estimated using photon and jet Monte Carlo (MC) samples and validated in data. Based on these studies, the efficiencies are parametrized as a function of the photon candidates' with 1.5% and 10% relative systematic uncertainties for and respectively. Having subtracted the estimated background from data in the muon channel, we estimate 947 40 (stat.) 16 (syst.) signal events when no requirement is applied, and 285 24 (stat.) 2 (syst.) signal events requiring GeV/.
As a cross-check, the jet background is also estimated through a fit to the shape of the distribution in data for both electron and muon channels, using MC templates constructed from simulated photon and jet events. The results are in good agreement with those obtained from the ratio and matrix methods.
Iv Results
iv.1 Total cross section
The total cross section for production is obtained from the ratio of the acceptance-corrected rate for GeV/, , GeV/, and , to the total acceptance-corrected dilepton rate for GeV/. Henceforth, these acceptance requirements are referred to as the generator-level requirements. We utilize this method because uncertainties associated with the trigger efficiencies, reconstruction efficiencies, and integrated luminosity are larger than the theoretical uncertainties and cancel in the ratio. This ratio is multiplied by a theoretical estimate for the total cross section for inclusive production for GeV/:
Here, and are the number of measured and background-subtracted events in the data sample, respectively. The factor is calculated with the fewz next-to-next-to-leading-order (NNLO) generator fewz1 -fewz2 , with the CTEQ6.6 parton distribution functions (PDF) CTEQ66 . The fewz theoretical prediction is 262.9 8.0 pb, where the dominant uncertainty is from the choice of PDF. The term is the branching fraction for , which in the SM is 3.4% for either electrons or muons. The factor corrects for the resolution effects that would cause events not to pass the selections on the generator-level quantities, e.g. a generator-level photon with GeV/, but to pass the reconstruction requirements, e.g. a reconstructed photon with GeV/. This factor is only used for events, and corrects for the photon energy smearing that dominates in the first bin. The muon resolution affects both and and the corresponding correction cancel in the ratio of cross sections. For the events that pass the generator-level requirements, the factors and provide the fraction of events that pass the analysis requirements, with all acceptances measured relative to the kinematic requirements at the generator level for the and final states, respectively. Events migrate between bins in because of finite detector resolution, and these effects are taken into account in calculating as a function of , while is calculated for the entire sample. To estimate and , we use inclusive events generated with the pythia pythia generator with final-state radiation simulated using photos photos and the CTEQ6.1L cteq61 PDF set. Because pythia is a leading-order (LO) generator and does not reproduce the observed spectrum in data, generated events are weighted to reflect the distribution observed in Ref. zpt . Events are then traced through the D0 detector using a simulation based on geant geant . Data events from random beam crossings are overlaid on the simulated interactions to reproduce the effects of multiple interactions and detector noise. Simulated interactions that take into account the observed differences between data and simulation are reweighted, e.g., the coordinate of the vertex, instantaneous luminosity, trigger efficiency, lepton identification (ID) efficiency, photon ID efficiency, and resolution effects. Here, the factor has values of 0.15 (0.17) in the electron channel (muon channel). When no constraints on are applied, the factor has average values of (stat.) and (stat.) for the electron and muon channels, respectively, and the average value of is 0.12 for both the electron and muon channels. Values for and are similar for the subsample requiring GeV/.
To account for systematic uncertainty on the migration into the sample from generated events with 10 GeV/, we conservatively vary the number of events produced outside the generator-level requirements in the pythia simulation by 20%, found as an upper estimate in studies of photon energy resolution in this kinematic regime, to measure the effect on the final cross section measurement. We find that the effect introduces a 1.5% systematic uncertainty on the total cross section. The dominant uncertainty corresponding to the calculation of is due to choice of the PDF set. There are 20 free parameters in the CTEQ6.1L parametrization of the PDF that reflect fits to data from previous experiments. The uncertainties on acceptance and efficiencies due to the PDF parametrization are estimated using the CTEQ6.1M PDF uncertainties, following Ref. PDFerrs . We find a total PDF uncertainty of 3.5%, dominated by the uncertainty on the acceptance-correction to the full geometrical lepton acceptance. The photon ID efficiency is determined from a simulated sample of photons and is estimated to have an uncertainty of 10% for 15 GeV/ and 3% for 15 GeV/.
To reduce the contribution of FSR in the data samples, we calculate the cross section with and without the GeV/ requirement. To combine the electron and muon channels, we utilize the method in Ref. BLUE , which averages the results of measurements with correlated systematic uncertainties. We assume the PDF and photon ID efficiency uncertainties to be 100% correlated between the two channels. The total cross section results can be found in Tables 1 and 2. The measurements are consistent with the NLO mcfm MCFM prediction using CTEQ6.6 PDF set CTEQ66 and the renormalization and factorization scales evaluated at the mass of the boson, GeV/. The PDF uncertainties associated with the SM prediction are evaluated following Ref. PDFerrs . We reevaluate the values for the spectrum calculated by NLO mcfm with the renormalization and factorization scales set to 160 GeV/ and again at 40 GeV/ and use these as estimates of the theoretical uncertainty of 1 standard deviation relative to the central NLO mcfm value.
|1026 62 (stat.) 60 (syst.)
|1158 53 (stat.) 70 (syst.)
|combined data
|1089 40 (stat.) 65 (syst.)
|NLO mcfm
|1096 34 (PDF) (scale)
|281 17 (stat.) 11 (syst.)
|306 28 (stat.) 11 (syst.)
|combined data
|288 15 (stat.) 11 (syst.)
|NLO mcfm
|294 10 (PDF) (scale)
iv.2 Differential cross section
We use the matrix inversion technique unfolding to unfold the experimental resolution and extract ( henceforth), the differential cross section for , as a function of the true . The elements of the smearing matrix between true and reconstructed bins are estimated using the full simulation of the detector response on a sample of events generated using pythia. Then, the matrix is inverted to obtain the unsmeared spectrum. We confirm that the unfolding procedure introduces a negligible bias. Following Ref. bincentering , the position of the data points are plotted in Figs. 3 and 4 at the value of where the cross section equals the average value for that bin. The theoretical uncertainties associated with the choice of PDF and the renormalization and factorization scales are determined analogously to the theoretical prediction for the total production cross section. The combined differential cross sections are shown in Figs. 3 and 4 for no requirement and GeV/, respectively. The values associated with Figs. 3 and 4 are given in Tables 3 and 4.
|combined data
|NLO mcfm
|111.14 4.40 (stat.) 11.99 (syst.)
|104.02 4.10 (PDF) (scale)
|51.41 3.83 (stat.) 2.65 (syst.)
|57.13 2.23 (PDF) (scale)
|25.34 2.74 (stat.) 1.13 (syst.)
|28.77 0.43 (PDF) (scale)
|8.08 1.45 (stat.) 0.40 (syst.)
|10.16 0.26 (PDF) (scale)
|3.23 0.60 (stat.) 0.17 (syst.)
|4.15 0.16 (PDF) (scale)
|1.70 0.26 (stat.) 0.088 (syst.)
|1.60 0.061 (PDF) (scale)
|0.34 0.079 (stat.) 0.018 (syst.)
|0.42 0.017 (PDF) (scale)
|0.038 0.014 (stat.) 0.002 (syst.)
|0.052 0.001 (PDF) (scale)
|combined data
|NLO mcfm
|13.57 1.87 (stat.) 2.43 (syst.)
|13.48 0.48 (PDF) (scale)
|14.87 2.17 (stat.) 2.30 (syst.)
|12.25 0.47 (PDF) (scale)
|7.91 1.76 (stat.) 0.81 (syst.)
|8.94 0.25 (PDF) (scale)
|5.30 1.15 (stat.) 0.44 (syst.)
|6.13 0.21(PDF) (scale)
|3.08 0.57 (stat.) 0.33 (syst.)
|3.71 0.15 (PDF) (scale)
|1.73 0.26 (stat.) 0.17 (syst.)
|1.57 0.061 (PDF) (scale)
|0.34 0.079 (stat.) 0.019 (syst.)
|0.42 0.017 (PDF) (scale)
|0.038 0.014 (stat.) 0.002 (syst.)
|0.052 0.001 (PDF) (scale)
|7.2 fb
|6.2 fb
|3.6 fb
V Limits on Anomalous Couplings
To set limits on anomalous trilinear gauge boson couplings, we generate events for different values of the anomalous couplings using the NLO Monte Carlo generator of Ref. baur . SM Drell-Yan production is included by reweighting the spectrum to mcfm for vanishing anomalous couplings. As shown in Fig. 5, anomalous couplings would contribute to an excess of high-energy photons as compared to the SM prediction. We apply the following generator-level requirements: GeV/, , GeV/, , and 110 GeV/, generate templates as a function of the anomalous couplings, and use the known acceptance and resolution functions to fold the predicted generator-level distribution into a reconstruction-level distribution for . Using Poisson statistics for GeV/, we define a likelihood function to compare the combined electron and muon channels with a predicted distribution for given values of anomalous couplings. In the absence of any significant deviation from the SM prediction, we set one-dimensional (1D) and two-dimensional (2D) limits on the anomalous coupling parameter values at the 95% C.L. A combined log-likelihood function using all data is defined by the sum of the individual log-likelihood functions of the electron and muon channels. We include the effect of systematic uncertainties associated with transforming a Monte Carlo template from the generator-level into a reconstructed distribution and find that these uncertainties contribute to the value of the calculated limits on the order of 1%. We generate a grid of templates for the distribution as a function of and for and , while setting all other coupling parameters to zero, and the limits are derived by varying about the maxima of the log-likelihood functions for the 95% C.L PDGstats . Results for the 1D limits for TeV and 1.5 TeV are shown in Table 5. The 1D and 2D limits on the anomalous coupling parameters are shown in Figs. 6 and 7, utilizing the electron and muon channels. In these figures, the dotted lines represent the theoretical limits on the anomalous coupling values, beyond which -matrix unitarity is violated. Because the parameters come from dimension-eight operators, the limits are more constrained than those of couplings, which are dimension-six.
We combine these results with those of a previous D0 analysis d0prev . In that analysis, the 1D and 2D limits on the anomalous couplings parameter were calculated using a data sample corresponding to an integrated luminosity of 1 fb of data collected between October 2002 and Feburary 2006 (3.6 fb of data collected between October 2002 and September 2008) in the and channels ( channel), for TeV. Results can be found in Fig. 8 and Table 5.
Vi Conclusions
We have measured the differential and total cross sections for production in collisions using the D0 detector at the Tevatron Collider with and without a GeV/ requirement. Both the total production cross sections and differential cross sections are consistent with the SM at NLO predicted by mcfm MCFM . We observe no deviation from SM predictions and place 1D and 2D limits on the -even anomalous couplings for and 1.5 TeV. When combining with the previous D0 analyses, the limits are comparable to those found in the most recent CDF result zgammaprev5 , which uses fb in the and channels and TeV. Our results include the first unfolded photon differential cross section , as well as the most precise measurement of the total production cross section of .
Acknowledgements.We thank the staffs at Fermilab and collaborating institutions, and acknowledge support from the DOE and NSF (USA); CEA and CNRS/IN2P3 (France); FASI, Rosatom and RFBR (Russia); CNPq, FAPERJ, FAPESP and FUNDUNESP (Brazil); DAE and DST (India); Colciencias (Colombia); CONACyT (Mexico); KRF and KOSEF (Korea); CONICET and UBACyT (Argentina); FOM (The Netherlands); STFC and the Royal Society (United Kingdom); MSMT and GACR (Czech Republic); CRC Program and NSERC (Canada); BMBF and DFG (Germany); SFI (Ireland); The Swedish Research Council (Sweden); and CAS and CNSF (China).
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'Ali ibn Ibrahim ibn al-Shatir al-Dimashqi (d. AH 777/1375 AD): Hashiyah 'ala al-mulakhas fi 'ilm al-falaq
Damascus, AH Rabi' I 801/11 Nov-9 Dec. 1398 AD
Astronomy, Arabic manuscript on cream paper, 73ff. with 19ll. of black naskh, occasional words and phrases in red, with several small diagrams, final folio with colophon signed Khalil ibn Haji Firoz al-Fardi and dated Rabi' I 801, in original tan morocco binding with flap, light staining and water damage
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INSIDE & OUT : DISCOVERIES : Furniture Forays : Shirt Lamps and Window Shelves
Who says functional furniture can't be fun? Not Dan Janotta and Marian Drahnak, the husband-and-wife team that created the Hawaiian Shirt Lamp and the Walking Window Display Case, pieces in their Janotta furniture line.
Frustrated by soaring prices and what they see as a lack of quality in furniture today, Janotta and Drahnak decided to come up with designs of their own, which are based on items like rocking horses, Hawaiian shirts and toasters.
The Hawaiian Shirt Lamp ($200) is made of solid mahogany, with a fishing lure for a pull switch. Janotta and Drahnak choose only colorful, uniquely patterned shirts for the lamps.
An open window is the idea behind the Walking Window Display Case ($1,700), which is a shelving unit that could also be used as a room divider. The shelves are attached to the frame in much the same way that blinds hang in a window.
All of the wood elements are maple and coated with an environmentally safe varnish. The legs and curtain rod are made of steel that has a satin silver powder coating. The plumb bob-shaped base is a necessary counterweight to balance the upper frame. The imported lace curtain is included.
Janotta and Drahnak--whose pieces are shown in art galleries in Los Angeles, San Diego, San Francisco and Ft. Lauderdale--opened their own studio in February in Hermosa Beach.
Janotta, 39, a senior architect for Johnson, Sand and Pereira Associates in Los Angeles, was a member of the team that designed the Orange County Performing Arts Center in Costa Mesa.
For more information or to order, call (310) 379-4051.
House Calls
Do you have deep scratches in your baby grand? A leg or two broken on your dining room table? Is the furniture too big to lug out the door?
It's not a problem for Roger Pigott, also known as the Finish Guy.
When you have larger pieces that you can't or don't want to move, Pigott, 33, of Poway, will come to your house to repair, touch up and finish your furniture.
Pigott, who averages between three and eight house calls a day, including an 18-chair job in Laguna Beach recently, specializes in repairing high-gloss lacquer finishes, such as those found on pianos and entertainment centers.
He started his mobile service for offices about 1 1/2 years ago, but his home-repair business has taken off, so he's concentrating on that end of the market. He also does work for antique and consignment shops.
Originally from El Segundo, Pigott has been in the repair business for 12 years.
His minimum varies depending on the distance, but the customer "gets an hour of advice or work, their choice," he says.
To reach the Finish Guy, call (619) 679-8837.
New Degrees of Leather
Traditional styling takes on a fresh look when paired with leather. A chair and ottoman from Natuzzi are made of a super-soft leather that looks and feels as smooth as butter. The chair and ottoman are typical of Natuzzi's lilt on furniture, using traditional themes and mixing them with leather in unexpected colors--such as banana yellow, butternut and lime green.
Pasquale Natuzzi, who is based in Italy, is the company's owner and principal designer. The company is the world's largest leather furniture manufacturer and offers more than 400 designs in leather.
The chair and ottoman, priced about $1,000, are available in Orange County at Moda Italia in Huntington Beach and at Plummers stores.


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Experience life above the trees ziplining just outside of Denali National Park! Your adventure begins with a three mile trail ride through the scenic Alaskan wilderness. After gearing up, certified guides will lead you along 6 sky bridges and 7 thrilling zip lines, including the dual racer finale! The built-in, hands-free braking system allows you to relax and enjoy the breathtaking mountain views. Challenge yourself by traversing to the top of the boreal forest on the uniquely designed Ascending Bridge Tower. Soar through the trees and over the tundra on over half a mile of ziplines. Complete this once in a lifetime experience by racing to the finish zipping along side your friends and family! All safety gear provided - full body harness, helmet, and gloves. Tour length is approximately 3 hours from pick-up to drop-off.
View this video for an overview!
"Take home awe-inspiring photographs of Alaska! With a maximum of 4 participants per group, you will receive a personalized photography experience featuring panoramic landscapes, majestic mountains, and reflection ponds. Our photo guides are professional photographers and expert light-wranglers; they will be your location scout, driver, and instructor – seeking out the best locations and the most dramatic lighting given the current weather conditions, light, and wildlife activity. The best camera is the one you have! Don't have one? Rent one from us! Our tour is designed to benefit all skill levels with any type of camera (smart-phones welcome). No matter what gear you have, our guides are experienced with all models of cameras & lenses and will be able to help you progress as photographer. Beginners will learn techniques to get more out of their equipment; how to read light and adjust their exposure settings to photograph Alaska's stunning scenery and wildlife in a way that "does it justice." Advanced photographers will enjoy the luxury of being driven to the best locations without having to rent a car or trying to scout the vast and unfamiliar landscape. Professional tripods and filters are provided. Digital cameras with long zoom lens are available to rent, and you keep the memory card. Tours are offered at times that are best for photography in our far north location. Check out our Midnight Sun tour - featuring long lasting sunset colors and alpenglow - and our new helicopter access backcountry photo excursion."
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The Denali Princess Wilderness Lodge is the closest and most comfortable place to stay when visiting the park. The entrance to Denali National Park is located only a mile from our front door. With an expansive deck overlooking the Nenana River with views into the park, Denali Princess Wilderness Lodge is the ideal spot to relax, visit with friends, and savor the exquisite landscape.
Family owned and operated since 1974, Denali Raft Adventures, Inc. is the original raft company on the Nenana River at the entrance of Denali National Park, Alaska. We offer Gore-Tex dry suits for the utmost in comfort, neoprene boots, Coast Guard approved lifejacket, and a guided 18ft raft which allows you to experience a sense of adventure and fun, while feeling safe. Choose the Denali rafting adventure thats right for you! Whitewater rafting or a scenic float down the Nenana River.
See our tour here!
Denali Rainbow Village RV Park, a Good Sam park, is the closest park to Denali National Park. It is located just 1 mile north of the park entrance. It is also within walking distance to all the shops, restaurants and tours in the Denali area. We have a very knowledgeable and helpful staff to assist you in ensuring your trip to Denali is truly magical. There are 55 full and partial hook-up sites available. All sites have 20 and 30 amp hook-ups. There are a limited number of 50 amp sites in both, full and partial hook-ups. Full hook-up sites are either back in or Pull thru. Each site has a picnic table, fire ring and access to free cable TV. The RV Park has a dump station, pay showers, laundry, clean restrooms, RV supplies & firewood. Pets are allowed in the RV park. All pets must be on a leash & guests must pick up after their pets immediately. Dog walking for a fee can be arraigned. Wi-Fi provided by Tengo Internet in the RV park. Receive 1/2 hour free Wi-Fi then a small fee is charged for more time.
Denali's Cannabis Cache is Denali's premier and only recreational retail marijuana store. Our boutique shop has a friendly and knowledgeable staff to help visitors select the right cannabis flower, edibles and concentrates to fit their needs. We provide a full shopping experience where locals, seasonal workers and travelers can purchase cannabis products, glass pipes, industry leading vaporizors, etc., along with clothing (hats, t-shirts, hoodies,) and other memorabilia to remember their time spent in Alaska and Denali National Park. Marijuana has intoxicating effects and may be habit forming and addictive; Marijuana impairs concentration, coordination and judgement. Do not operate a vehicle or machinery under its influence; There are health risks associated with the consumption of marijuana; For use only by adults 21 years of age and older. Keep out of the reach of children; Marijuana should not be used by women who are pregnant or breastfeeding.
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