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In January this year, the construction company HOCHTIEF VSB submitted a request for certification of the Management System of Safety and Health Protection at Work (BOZP) and on May 2nd, 2005 the company received a certificate issued by the certification body STAVCERT Prague, which confirms that HOCHTIEF VSB has an implemented and maintained the Management System of Safety and Health Protection at Work, which corresponds to the requirements of OHSAS 18001:1999.
The very short period that had passed from submission of the request to the actual reception of the certificate was preconditioned by a high demand on the entire execution team, existence of the Safe Enterprise certificate and most of all by the ability of management employees to react to the comments of the certification body arising from the pre-audit. Revision of all steering documentation in the sphere of the BOZP was executed, technical and organizational procedures vital for safety management systems were newly elaborated. Working regulations, emergency plans, machinery and mechanization maintenance plans were newly incorporated or elaborated.
The certification audit itself took place on two levels. Within the first level (pre-audit) the auditors acquainted themselves with the implementation of the BOZP Management System and formulated their findings, which were to be removed. Within the second level (certification audit), auditors verified, besides the removal of findings, also the entire BOZP Management System. Within the final discussion the auditors appreciated the high level of BOZP in our company, helpful and professional approach of all employees and stated that the BOZP Management System in our company corresponds with requirements of OHSAS 18001:1999 and it is possible to issue a certificate.
The OHSAS 18001:1999 Standard is fully compatible with the Quality Management System according to ČSN EN ISO 9001:2001 and with the Environmental Management System according to ČSN EN ISO 14001, which are also held by the company. By gaining of the certificate according to the OHSAS 18001:1999, the company clearly expressed that working conditions, working environment and health protection for employees are not merely an obligation stipulated by the law, but also a reality which the company perceives as given.


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VCU Links
Virginia Sports
Cavalier Swim
UVA Swim Page
Contact Kerry Smith
cavalierswimcamps@gmail.com
Todd DeSorbo
Tyler Fenwick
Blaire Bachman
Wes Foltz
ANDREW SHEAFF
Todd DeSorbo Head Coach
Todd DeSorbo was hired as the head men's and women's swimming and diving coach in August 2017. He joins the UVA staff after serving on the staff at NC State the past six seasons as the associate head coach.
At NC State, DeSorbo worked primarily with the Wolfpack sprinters and was a developmental specialist. He oversaw the programs' recruiting, training and day-to-day operations.
During his tenure at NC State, DeSorbo coached American Olympic gold medalist Ryan Held (2016 Rio 4x100 free relay), USA Swimming national champion Justin Ress and NCAA Champions in the 4x100 free relay (2016) and 4x200 free relay (2017).The NC State men won the last three ACC titles and the Wolfpack women captured the 2017 ACC title. Both NC State programs produced their highest finishes at the NCAA Championships this past season. The Wolfpack men placed fourth overall while the women's team finished seventh.
In 2017, his athletes earned seven individual ACC titles and garnered 14 All-ACC honors, helping to lead both programs to sweep their respective ACC Championships meets. Additionally, DeSorbo coached 13 athletes to the 2017 NCAA Championships where they collected over 30 All-America honors on the way to the teams highest NCAA finishes in program history.
On the men's side, he led sprint standout Held to three top-eight individual performances at NCAAs, highlighted by a runner-up title in the 50 freestyle in a time of 18.60. Andreas Vaziaos also tabbed three top-eight finishes, his highest being fifth in the 200 butterfly with a conference record and school record of 1:40.80.
Tyler Fenwick Associate Head Coach
Tyler Fenwick joined the UVA coaching staff in August 2017 as the men's and women's associate head coach.
Fenwick served as the associate head coach at Tennessee from 2012-2017. During his time with the Volunteers, he coached four U.S. Olympians, 200 All-Americans and saw his student-athletes set 36 school records.
Prior to Tennessee, Fenwick coached the men's national team at the Mission Viejo Nadadores in Mission Viejo, Calif., as a senior coach. While working with the U.S. national team, Fenwick coached two 2012 FINA world junior champions, the 2012 U.S. Open Water men's national champion, one U.S. national champion and one U.S. junior national champion.
Fenwick served as the assistant coach for Germantown Academy Aquatic Club in Fort Washington, Pa., from 2004-07 and the assistant coach for the University of Tennessee Aquatics program from 2007-09.
Blaire Bachman Assistant Coach
Blaire Bachman joined the UVA coaching staff in August 2017 as an assistant coach.
Bachman worked as the assistant swimming coach and women's recruiting coordinator for Indiana from 2016-17. Her primary responsibility was to recruit and assist with the middle distance and distance training groups.
Prior to working at Indiana, Bachman spent a year as the assistant swimming coach and women's recruiting coordinator for Dartmouth. From 2010-15, she worked as the head swimming coach at Brenau University administering year-round training.
Bachman started her coaching career as a camp counselor and coach for the Georgia Bulldogs Swim Club (2012-2016).
Wes Foltz Assistant Coach
Wes Foltz was named a Virginia swimming assistant coach in August 2017.
Foltz served as an assistant coach at NC State in 2016-17, helping the program achieve one of its best performances in recent history. Foltz helped coach 34 male and 25 female All-American performances as well as aiding both programs to a top-10 NCAA finish. Additionally, he had a hand in the Pro Group Wolfpack Elite's success over the last year including a World Championship title by Simonas Bilis and a third-place finish for Cullen Jones at the 2017 U.S. World Championship Trials.
Prior to NC State, Foltz worked at Southern California (2014-16) as the assistant coach, helping the program record 64 All-American performances. During this time, the women's program captured the 2016 Pac-12 conference championship and a sixth-place finish at the NCAAs. The men's team recorded the conference title in 2015 in addition to finishing fourth at the NCAAs.
From 2012-15, Foltz was a volunteer assistant coach for NC State in addition to working with the Marlins of Raleigh swim team (2012-14) as an assistant coach.
ANDREW SHEAFF Assistant Coach
Andrew Sheaff is serving in his first year as an assistant coach for the Virginia men's and women's swimming and diving team, joining the staff in April 2018.
Sheaff was a volunteer coach with Virginia during the 2017-18 season, working alongside the current staff in DeSorbo's first year as the head coach of the program. With the help of Sheaff, the Cavaliers recorded nine school records and five ACC titles in addition to seeing 60 performances rank in the top 10 on Virginia's all-time list. Sheaff aided the program in administrative tasks and assisted in planning and execution of daily training.
Prior to Virginia, Sheaff served as the associate head coach for Northwestern men's swimming team from 2012-17. During his five-year stint with the Wildcats, Sheaff developed programming focused on fostering a positive team atmosphere and culture. He established and designed dryland training for all team members with specific training for the team's sprinters.
From 2009-12, Sheaff served as an assistant coach at Bucknell where he worked with the team's sprinters and breaststrokers. Sheaff also coached at the Bison Aquatic Club from 2010-12, aiding in the development of age-group swimmers.
Sheaff began his coaching career at Maryland, serving as a volunteer assistant from 2007-09.
Sheaff has an extensive background in strength in conditioning. In 2007, he worked as an intern at Pittsburgh before interning with the Cleveland Browns throughout the summer. Sheaff worked alongside elite training staff, learning different programming techniques for developing advanced training programs.
A collegiate swimmer at Pittsburgh, Sheaff was named the Senior Athlete of Distinction. He was a four-time Big East Academic All-Star and a four-time University Scholar Athlete.
Sheaff has a bachelor of science in exercise science from Pittsburgh and a masters in exercise physiology from Maryland.
***In accordance with the rules of the NCAA the camps are open to all swimmers but each camp will be limited by number of participants.
***In accordance with the rules of the NCAA we are prohibited to give free/reduced camps to prospects.
Site design, hosting, and online registration services provided by SDI Camps

redpajama_set_name: RedPajamaCommonCrawl


Lately, Ty and I have been doing a lot of thinking, reviewing, and finessing our Vision and Mission statements. As a Creative, it's tempting to launch into business with a motivation of, "I want to make beautiful things!" but that's actually not best practice. It took me (honestly) probably ten years to realize that 'me making beautiful things' is all about, well, me. A good business isn't about me—it's about you, the client, customer, audience, community.
Over the last few years, I've been more intent on listening, and learning. The truth is this: name any product you want to purchase and you can probably also name at least four places where you can purchase it. Invitations are no different. We create beautiful invitations, but so do other artists and stationers all over the country. I sit across the consultation table from clients all the time, and I'm listening: What do they really need? Why are they here? And the answer may surprise you: it isn't that they want invitations. What we are actually offering here at The Happy Envelope is Peace of Mind.
We take the confusion out of ordering invitations. We are your guide so that you can move forward with confidence: in the beauty of the finished product, in the wording, in proper etiquette, in clarity of pricing and budget, in the manner of printing… I am literally holding your hand and walking side by side as your guide. Yesterday, a bride picked up her invitations and said, "I love them! And this was so much easier than I thought it would be." That's my job, and I love it. Nothing makes me happier than a stress-free bride.
So, I've been tackling this role of Guide. A good guide leads—not by charging ahead as you scurry to keep up. A good guide explains as they lead. They are imparting understanding and education as they go. If you take a guided tour through Paris, you'd want to enjoy the journey and leave with a better understanding of Paris, its history, culture, and what it offers today.
And if you're in the season of pulling together a rock star wedding team, look no further than these experts!
I wish that couples knew before and during the planning process that the wedding is about the two of them and their families joining together. It's a celebration of all your loved ones from all walks of life getting together, and you get to be creative and enjoy hosting everyone you love in one place! If you keep it light and tune out the buzz of everyone else's ideas of what you SHOULD be doing, you won't lose sight of the fun and joy of your wedding weekend. Above all else, be present.
As a planner, of course I wish the couple knew from the start that they shouldn't "go it alone" when planning their wedding. Having an experienced planner they can trust with their vision and the details will allow them to enjoy the process and focus on what is most important: their relationship and the marriage they are entering into!
I'd like brides to be focused on making a real connection with their vendors. When it comes to the beauty team (hair + makeup), make sure that your vision is truly heard and understood, rather than being overly concerned with details like the methods of application, pricing, or specific brands that might be used. Yes, details are important, but a unified vision and trust level should be established first and foremost. If a makeup artist uses a brand of makeup that you like, but you can't connect with her or she can't execute your vision, those details won't matter. If an artist is inexpensive and fits your budget but doesn't connect well with you or your vision, it's simply not going to work. You want your end result to be beyond what you expected!
I wish that brides would think about how they are going to address their envelopes before they actually need them addressed. Book your calligrapher at the same time you begin ordering your invitations. Calligraphers book quickly and early… and we only have one writing hand! Your stationer and calligrapher can work together to create a cohesive presentation for your guest's first exposure to your wedding.
One thing a couple needs to know before they can begin planning their wedding would be… THEIR BUDGET.
Vendors are able to guide couples through their wedding planning much easier if they know their budget. As a florist, we can direct them in the things they NEED, and not what they WANT to keep them in the budget. We can substitute more cost-effective flowers to get the look they love for less money to keep them in budget if we know it going into the first consultation.
Brides may not realize how much time they will spend with their vendors. Thus, they not only need to work with people whose product/service they enjoy but also who they connect with on a personal level. Weddings can be stressful and they need someone in their lives who is constant, organized, and who brings out the best in them. At the end of the day, your vendors' first priority should be to serve you and help set you up for a wonderful marriage!


Appreciating good food and wine is an intrinsic part of being French. To this effect, it almost comes as a surprise that it is only recently the French have instituted a festival around this – Fête de la Gastronomie. This is the first but am sure the trend, once set, will only grow bigger in years to come.
For three days, 20-22 September 2013, the country will turn into one giant centre for showcasing their culinary prowess. Not that they don't like to show off otherwise but this is more about good eating than merely good publicity. Although the entire industry of food will be involved in some manner, what is of particular interest is that 27 noted chefs representing 27 regions of France (even I didn't know that there were that many with marked differences) will prepare and showcase recipes for five Euros, (yep you read that right) for people to take home and try. I do wish they'd prepare the menu too; I'd even pay a whole extra Euro for the trouble. For others (like me) who don't wish to put in the effort, there are huge banquets being organised in most regions where people can attend and indulge in some communal grubbing. Other things being organised include picnics and food trails. Some of these would lead into the heart of French gastronomy, from visits to chef's kitchens to farms amd laboratories – the entire diaspora of the country's kitchen repertoire will be available to the curious few who wish to explore.
In fact, almost in-keeping with the tradition of French rivalry, each region is out to showcase the best of their part of the world. And in a country which counts some of the top wines and cuisines of the world among its many regional specialities one can only imagine how rife must the air be with this undeclared culinary competition. And then am sure the local wines will play an important part in this too.
Not just in France but this French gastronomy festival is being celebrated in countries as far as Argentina as well. In India, I don't know if we are doing anything but I for sure will head out for a nice French meal. The options in the capital (purely in order of distance from my house) – Le Bistro du Parc, Chez Nini, Le Cirque, and Rara Avis. If there is any other French restaurant worth its Bechamel that I have left out, please leave me a note here.


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How to check if a phone is stolen
If you are buying a used phone you should always check its status to make sure it hasn't been reported as lost or stolen. Some…
November 6, 2020 • By Robert Nelson
How to check if an iPhone is stolen
When you're considering buying or selling a used iPhone, you should find out if it's been reported as lost or stolen. An iPhone that has…
What is the difference between MEID and IMEI?
Every cellular-connected device has a unique serial number. These are most commonly seen on smartphones; however, unique identifiers are also present on cellular-enabled tablets, smartwatches,…
October 30, 2020 • By Robert Nelson
Check your IMEI, ESN, and MEID for free on Swappa
One of the many tools we use to keep the Swappa community safe is our free IMEI check. Although it's just one piece of the puzzle, it sets us apart from sites like eBay. We recently updated our free IMEI check with several new features.
October 2, 2020 • By Will Verduzco
A brief guide to IMEI, ESN, and other numbers on your phone
All mobile phones, as well as other cellular-connected devices such as tablets, have a unique serial number. There have been a few different names and…
September 14, 2020 • By Robert Nelson
Why are bad ESN devices allowed to be sold on the Boneyard?
The idea for Boneyard came primarily from legitimate business sellers and re-sellers that wanted to be able to sell all of their devices, even the…
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ABC, coming off the highs and lows of the extraordinary ratings success of the Roseanne revival and the turmoil after its abrupt cancellation, is heading into next season with four new comedy series: the Roseanne spinoff The Conners, two more family comedies, The Kids Are Alright and Single Parents, and one more spinoff, The Goldbergs sequel Schooled; as well as five dramas, ensemble A Million Little Things, soap Grand Hotel, legal drama The Fix and light procedurals The Rookie and Whiskey Cavalier.
But as the broadcast networks are gearing up for fall 2018 launch, they are also looking ahead as they begin to buy pitches for the 2019-20 season.
In an interview with Deadline during TCA, ABC Entertainment president Channing Dungey talks about the network's development targets in drama and comedy and gives a status update on The Middle spinoff and two pilots from last season, which were kept alive for redevelopment, drama False Profits and comedy Steps.
Multi-generational family dramas are a priority.
On the comedy side, ABC plans to largely stay in its lane while widening that lane a bit.
ABC previously explored millennial themes with the black-ish spinoff grown-ish, which was piloted at ABC before moving to Freeform.
Comedy spinoffs have definitely been part of ABC's MO the last few years, with black-ish, The Goldbergs and now Roseanne all getting spinoff series. Another high-profile comedy spinoff, from long-running The Middle, also is in the works.
The project, starring series co-star Eden Sher, from the original series' creators/executive producers Eileen Heisler and DeAnn Heline and studio Warner Bros. TV, has a pilot production commitment. Because of the pedigree and the auspices, the spinoff is expected to get a greenlight but that is still ways off. Dungey said she will be hearing a pitch for the show this week.
Both projects extended the options on cast members, and False Profits in May also received an order for backup scripts.
Overall. Dungey expects to buy a number of pitches in line with last year. And despite the rocky experience on Roseanne, she remains open to reboots with some caveat.
Will ABC try to do more comedies focused on that segment of the population, Middle America?
"It's too early to tell but we have had that as a priority on both sides, comedy and drama," Dungey said.


text:
Aprosencephaly: Review of the literature and report of a case with cerebellar hypoplasia, pigmented epithelial cyst and Rathke's cleft cyst
T. S. Kim, S. Cho, Dennis W Dickson
Aprosencephaly is a very rare brain malformation that occurs in isolated and sydromatic forms. The syndromatic form has been named "XK-aprosencephaly", and is characterized by near total absence of prosencephalon with a midline oculofacial defect similar to the most severe forms of holoprosencephaly, in association with limb and genital anomalies. We present a case of syndromatic aprosencephaly with absence of thumb and abnormal external genitalia. A previously undescribed finding was a Tathke's cleft cyst. Two other cystic structure were also identified - an ependymal cyst, which may represent a dorsal cyst as in holoprosencephaly, and a pigmented epithelial cyst, which may represent a rudimentary eye. Additional findings were extensive calcific vasculopathy in the rudimentary prosencephalon, absence of pituitary gland, forking of the aqueduct of Sylvius and marked cerebellar hypoplasia. Since calcific vasculopathy is a common accompaniment of other inflammatory diseases of the central nervous system, its presence in this case suggests that destructive processes may be involved in the genesis of some cases of aprosencephaly.
Acta Neuropathologica
Aprosencephaly
Glio-ependymal cyst
Pigmented epithelial cyst
Rathke's cleft cyst
Dive into the research topics of 'Aprosencephaly: Review of the literature and report of a case with cerebellar hypoplasia, pigmented epithelial cyst and Rathke's cleft cyst'. Together they form a unique fingerprint.
Central Nervous System Cysts Medicine & Life Sciences 100%
Cerebellar Hypoplasia Medicine & Life Sciences 99%
Anencephaly Medicine & Life Sciences 94%
Holoprosencephaly Medicine & Life Sciences 47%
XK aprosencephaly Medicine & Life Sciences 35%
Prosencephalon Medicine & Life Sciences 34%
Genitalia Medicine & Life Sciences 30%
Kim, T. S., Cho, S., & Dickson, D. W. (1990). Aprosencephaly: Review of the literature and report of a case with cerebellar hypoplasia, pigmented epithelial cyst and Rathke's cleft cyst. Acta Neuropathologica, 79(4), 424-431. https://doi.org/10.1007/BF00308719
Aprosencephaly : Review of the literature and report of a case with cerebellar hypoplasia, pigmented epithelial cyst and Rathke's cleft cyst. / Kim, T. S.; Cho, S.; Dickson, Dennis W.
In: Acta Neuropathologica, Vol. 79, No. 4, 01.1990, p. 424-431.
Kim, TS, Cho, S & Dickson, DW 1990, 'Aprosencephaly: Review of the literature and report of a case with cerebellar hypoplasia, pigmented epithelial cyst and Rathke's cleft cyst', Acta Neuropathologica, vol. 79, no. 4, pp. 424-431. https://doi.org/10.1007/BF00308719
Kim TS, Cho S, Dickson DW. Aprosencephaly: Review of the literature and report of a case with cerebellar hypoplasia, pigmented epithelial cyst and Rathke's cleft cyst. Acta Neuropathologica. 1990 Jan;79(4):424-431. doi: 10.1007/BF00308719
Kim, T. S. ; Cho, S. ; Dickson, Dennis W. / Aprosencephaly : Review of the literature and report of a case with cerebellar hypoplasia, pigmented epithelial cyst and Rathke's cleft cyst. In: Acta Neuropathologica. 1990 ; Vol. 79, No. 4. pp. 424-431.
@article{214de5529c0d4484818c2d1d56f38445,
title = "Aprosencephaly: Review of the literature and report of a case with cerebellar hypoplasia, pigmented epithelial cyst and Rathke's cleft cyst",
abstract = "Aprosencephaly is a very rare brain malformation that occurs in isolated and sydromatic forms. The syndromatic form has been named {"}XK-aprosencephaly{"}, and is characterized by near total absence of prosencephalon with a midline oculofacial defect similar to the most severe forms of holoprosencephaly, in association with limb and genital anomalies. We present a case of syndromatic aprosencephaly with absence of thumb and abnormal external genitalia. A previously undescribed finding was a Tathke's cleft cyst. Two other cystic structure were also identified - an ependymal cyst, which may represent a dorsal cyst as in holoprosencephaly, and a pigmented epithelial cyst, which may represent a rudimentary eye. Additional findings were extensive calcific vasculopathy in the rudimentary prosencephalon, absence of pituitary gland, forking of the aqueduct of Sylvius and marked cerebellar hypoplasia. Since calcific vasculopathy is a common accompaniment of other inflammatory diseases of the central nervous system, its presence in this case suggests that destructive processes may be involved in the genesis of some cases of aprosencephaly.",
keywords = "Aprosencephaly, Glio-ependymal cyst, Pigmented epithelial cyst, Rathke's cleft cyst",
author = "Kim, {T. S.} and S. Cho and Dickson, {Dennis W}",
journal = "Acta Neuropathologica",
T1 - Aprosencephaly
T2 - Review of the literature and report of a case with cerebellar hypoplasia, pigmented epithelial cyst and Rathke's cleft cyst
AU - Kim, T. S.
AU - Cho, S.
AU - Dickson, Dennis W
N2 - Aprosencephaly is a very rare brain malformation that occurs in isolated and sydromatic forms. The syndromatic form has been named "XK-aprosencephaly", and is characterized by near total absence of prosencephalon with a midline oculofacial defect similar to the most severe forms of holoprosencephaly, in association with limb and genital anomalies. We present a case of syndromatic aprosencephaly with absence of thumb and abnormal external genitalia. A previously undescribed finding was a Tathke's cleft cyst. Two other cystic structure were also identified - an ependymal cyst, which may represent a dorsal cyst as in holoprosencephaly, and a pigmented epithelial cyst, which may represent a rudimentary eye. Additional findings were extensive calcific vasculopathy in the rudimentary prosencephalon, absence of pituitary gland, forking of the aqueduct of Sylvius and marked cerebellar hypoplasia. Since calcific vasculopathy is a common accompaniment of other inflammatory diseases of the central nervous system, its presence in this case suggests that destructive processes may be involved in the genesis of some cases of aprosencephaly.
AB - Aprosencephaly is a very rare brain malformation that occurs in isolated and sydromatic forms. The syndromatic form has been named "XK-aprosencephaly", and is characterized by near total absence of prosencephalon with a midline oculofacial defect similar to the most severe forms of holoprosencephaly, in association with limb and genital anomalies. We present a case of syndromatic aprosencephaly with absence of thumb and abnormal external genitalia. A previously undescribed finding was a Tathke's cleft cyst. Two other cystic structure were also identified - an ependymal cyst, which may represent a dorsal cyst as in holoprosencephaly, and a pigmented epithelial cyst, which may represent a rudimentary eye. Additional findings were extensive calcific vasculopathy in the rudimentary prosencephalon, absence of pituitary gland, forking of the aqueduct of Sylvius and marked cerebellar hypoplasia. Since calcific vasculopathy is a common accompaniment of other inflammatory diseases of the central nervous system, its presence in this case suggests that destructive processes may be involved in the genesis of some cases of aprosencephaly.
KW - Aprosencephaly
KW - Glio-ependymal cyst
KW - Pigmented epithelial cyst
KW - Rathke's cleft cyst
JO - Acta Neuropathologica
JF - Acta Neuropathologica


If selected, horizontal/vertical axis coordinates are logarithmic, otherwise they are linear.
If selected, horizontal/vertical axis coordinate axes run in the opposite direction to normal.
If selected, the number of pixels per unit is always the same on both axes, i.e. the unit square is always a square. Otherwise, there is no constraint on the relative sizes of the X and Y axis units.
Normally, dragging with the left/right mouse buttons or using the mouse wheel on the main part of the plot will pan/zoom it in both X and Y directions. By unchecking the X or Y checkbox here, you can prevent pan/zoom in the corresponding direction, so if the Y box is unchecked, pan/zoom will only affect the vertical direction (note the same effect can be achieved by dragging to the left of the Y axis).
Normally, zoom operations zoom around the position of the mouse at the start of the wheel/drag gesture. Checking these boxes fixes the X/Y reference coordinate for zooms to be the Y=0 or X=0 lines. This can be useful if you want the X or Y axis to stay put (e.g. at the edge of the plot) during zoom actions.
Controls the factor by which each zoom action zooms the plot. Moving this slider to the left/right makes the mouse more/less sensitive (one wheel click or dragging a fixed distance has more/less zoom effect).
The Range tab provides manual configuration of the visible range of the plot. Making changes to this tab will reset the visible plot range, but not vice versa - zooming and panning in the usual way will not change the settings of this panel.
Filling in the Minimum/Maximum fields for either or both axes will constrain the corresponding range of the visible data. The limits corresponding to any of those fields that are left blank will initially be worked out from the data. The Subrange double-sliders restrict the ranges within the (explicit or automatic) min/max ranges. Note you can move both sliders at once by grabbing a position between the two.
The Clear button resets all the fields. The Submit button updates the plot with the current values in this tab, as does making any changes to it.
If true, grid lines will be drawn across the plot for every tick mark.
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If set, minor (unlabelled) tick marks will be drawn between the major (labelled) ones.
Use the slider to influence how many tick marks are draw on each axis.
The Labels tab controls the text labels on the axes. If the Auto checkbox is set, the text will be taken from one of the data coordinates being plotted on that axis. To override those with your own axis labels, unset Auto and type text in to the Label fields.
The Font tab configures the font used for axis annotation. It also affects some other things like the legend.
How to turn the text into characters on the screen. Plain and Antialias both take the text at face value, but Antialias smooths the characters. Antialiased text usually looks nicer, but can be perceptibly slower to plot. At time of writing, on MacOS antialiased text seems to be required to stop the writing coming out upside-down for non-horizontal text. LaTeX interprets the text as LaTeX source code and typesets it accordingly.
Size of the font in points.
Whether the font is plain, bold or italic.


Prepare yourself for a trip through time to the period of Ancient Egypt in Play'n Go's Legacy of Egypt slot which, despite the thoroughly played out Egyptian theme, has a bunch of sharp visuals and the power to award cash wins that could leave you feeling like a pharaoh all from the comfort of your home.
Legacy of Egypt is a 5 reel, 30 payline video slot that's set in the desert kingdom in front of an ancient temple. The game is riddled with paint and gold, and you get the feeling that you can live the life of a God if you hit it big. The game's symbols are well done and include standard slot icons (J, Q, K, A) as well as the Pharaoh and Queen and an array of gods: Bastet the cat god, Sobek the crocodile god, Anubis the dog god, and Horus the falcon god. You can also find a pyramid that rotates on three different tiers which is the game's scatter symbol.
Features in the Legacy of Egypt include a wild scatter, a wheel of fortune that applies free spins and win multipliers, standard wilds, and standard scatters. The features here actually seem to hit quite frequently, so you're likely to score some frequent mid sized wins while testing your luck.
As much as I enjoyed the gameplay features, I have to praise the visual presentation just as much. The game looks so sharp and is just well done, unlike many of the other slot machines we see from other developers these days. When speaking about the presentation, you also have to mention the mobile version of the game, which looks sharp and is stunning on smaller devices such as smartphones.
There have been so many Ancient Egyptian slot machines released over the years that they largely blend together. Once in a while though, we get a game like Legacy of Egypt that stands heads and shoulders above the competition, and I highly recommend you give it a spin.
I have a love-hate ship with this game. It can pay well and it can be easy to retrigger the bonus round, but my best win so far has been around 200x bet win with many retriggers. When it's in a bad run- beware!
I like the free spin feature itself of this game. The win can be huge in the way the free spin feature is made. But, I kind of doubt if it can give really big wins. My best win was only 200~300x bet from any of Play N'Go slots.
I played this game with real money some days ago, but I got only like 50~70x bet from the free spin, huh.


Portable Garage Shelter offers replacement covers for fabric covered portable shelters, carports, garages, canopies, fabric sheds, hoop buildings, and tents. View our Youtube videos which indicate the required measurements for a replacement cover and end panel. https://www.youtube.com/watch?v=mLpG6V_va68 We also demonstrate how to install a replacement cover. https://www.youtube.com/watch?v=ngSJeWFQ8_k&t=30s Our replacement covers are manufactured from woven 12.5 oz/ square yard 24 mil polyethylene which is thermally sealed at the seams for a watertight seal. Replacement covers are 100% manufactured in the USA with quality materials, high tech equipment and quality workmanship. All replacement covers include ratchets, straps, and conduit pipe which inserts into the cover pocket. A 15 year manufacturer prorated warranty is included with these heavy duty covers. Color options include: green, tan, white, and gray. The following FRAME measurements are required to obtain a price quote for the replacement cover on all shelters and canopies (all measurements must be in inches). Please do NOT provide cover dimensions.
1.) Frame width (open end); 2.) Frame length; 3.) Frame height to top center; 4.) Distance around arch or A frame shape (ground to ground); do not provide wall height measurements if structure is mounted on a wall, if roof top only is needed, please provide roof measurements; 5.) Frame distance between legs (center to center); 6.) Frame pipe diameter; 7.) Shelter shape (round, A frame, or barn style); 8.) Desired color (white, green, tan, red, or gray); 9.) Mounting arrangement (asphalt, concrete pad, block wall, wood wall, etc); 10.) End panel requirements (if needed); zippered door width x height (note that zipper heights are in increments of 2'); 11.) Customer contact and phone number; 12.) Complete shipping address.
Photos of the current shelter are encouraged to support in obtaining the proper product. Portable Garage Shelter is not responsible for incorrect measurements provided by the customer.


text:
Pierre Perrier (1935-), ingénieur français ;
 Pierre Perrier (1984-), acteur français.

redpajama_set_name: RedPajamaWikipedia


text:
import unittest
import json
import os
from dagda.analysis.static.dependencies.dep_info_extractor import get_filtered_dependencies_info
from dagda.analysis.static.dependencies.dep_info_extractor import read_4depcheck_output_file

# -- Test suite

class DepInfoExtractorTestSuite(unittest.TestCase):

    def test_raw_info_to_json_array(self):
        filtered_dep = get_filtered_dependencies_info(json.loads(mock_json_array), '/tmp/sdgas68kg')
        self.assertEqual(len(filtered_dep), 3)
        self.assertTrue('python#lxml#1.0.1#/tmp/lxml.1.0.1.py' in filtered_dep)
        self.assertTrue('java#cxf#2.6.0#/tmp/cxf.2.6.0.jar' in filtered_dep)
        self.assertTrue('java#navigator#4.08#/tmp/navigator.4.08.jar' in filtered_dep)

    def test_read_4depcheck_output_file_exception(self):
        msg = ''
        try:
            read_4depcheck_output_file('no_image_name')
        except Exception as ex:
            msg = ex.get_message()
        self.assertEqual(msg, '4depcheck output file [/tmp/4depcheck/no_image_name.json] not found.')

    def test_read_4depcheck_empty_output_file(self):
        # Prepare test
        try:
            os.makedirs('/tmp/4depcheck')
            created = True
        except OSError:
            created = False
        with open('/tmp/4depcheck/empty_output_file.json', 'w') as f:
            None
        # Run
        raw_info = read_4depcheck_output_file('empty_output_file')
        # Clean up
        os.remove('/tmp/4depcheck/empty_output_file.json')
        if created:
            os.removedirs('/tmp/4depcheck')
        # Check
        self.assertEqual(raw_info, '')

# -- Mock Constants

mock_json_array = '[{"cve_type": "python", "cve_product": "lxml", "cve_product_version": "1.0.1", "cve_product_file_path": "/tmp/lxml.1.0.1.py"}, {"cve_type": "java", "cve_product": "cxf", "cve_product_version": "2.6.0", "cve_product_file_path": "/tmp/cxf.2.6.0.jar"}, {"cve_type": "java", "cve_product": "navigator", "cve_product_version": "4.08", "cve_product_file_path": "/tmp/navigator.4.08.jar"}]'

if __name__ == '__main__':
    unittest.main()

redpajama_set_name: RedPajamaGithub


text:
A Purpose-Driven Life - Steve Rodgers
podcast Sep 23, 2020
Steve Rodgers is a former Warren Buffett CEO who experienced a radical spiritual transformation that has evolved into a new mission as a purpose-driven consultant and entrepreneur coach, in-demand international keynote speaker, and bestselling author. He specializes in helping business owners and leaders increase profits while bringing spiritual intelligence into every aspect of their personal and professional lives to invite in success, fulfillment, and abundance beyond their wildest dreams.
Steve and Mark talk about boldness, life as a game of Whack-A-Mole, intentionality, having a personal balance sheet, life plan maps, why you're here, how to embrace quiet, and more!
His website


text:
La estación de Weinfelden es la principal estación ferroviaria de la comuna suiza de Weinfelden, en el Cantón de Turgovia.

Historia

La primera estación de Weinfelden fue abierta en el año 1855 con la apertura al tráfico ferroviario de la línea que unía a Winterthur con Romanshorn, del Schweizerische Nordostbahn (NOB). El edificio de la estación terminó de construirse en los años 1863 - 1864. En 1911 se inauguró el conocido como Mittelthurgaubahn, que parte desde Wil hasta Kreuzlingen.

Situación

La estación se encuentra ubicada en el centro del núcleo urbano de Weinfelden. Tiene un total de tres andenes, de los cuales uno es central y los otros dos son laterales a los que acceden cuatro vías. Hay que sumar la existencia de otra vías pasante y varios haces de vías muertas.

La estación está situada en términos ferroviarios en la línea férrea Winterthur - Romanshorn, y en la línea Wil - Weinfelden - Kreuzlingen. Sus dependencias ferroviarias colaterales son la estación de Märstetten hacia Winterthur, la estación de Bussnang en dirección Wil, la estación de Kehlhof hacia Kreuzlingen y la estación de Bürglen en dirección Romanshorn.

Servicios ferroviarios

Los servicios son prestados por SBB-CFF-FFS, que ofrece conexiones de larga distancia, regionales y de cercanías:

Larga distancia

  Romanshorn - Amriswil - Sulgen - Weinfelden - Frauenfeld - Winterthur - Zúrich Aeropuerto - Zúrich - Berna - Thun - Spiez - Visp - Brig.
  Biel/Bienne - Grenchen Süd - Soleura - Oensingen - Olten - Zúrich - Zúrich Aeropuerto - Winterthur - Frauenfeld - Weinfelden - Kreuzlingen - Constanza. Trenes cada hora por dirección.

Regional

  Weinfelden - Wil.
  Weinfelden - Kreuzlingen - Constanza.

S-Bahn
S-Bahn San Galo
A la estación llegan dos líneas de la red de cercanías S-Bahn San Galo:
  San Galo – Gossau – Weinfelden. Trenes con frecuencias cada hora.
  Weinfelden – Sulgen – Romanshorn - Rorschach.

S-Bahn Zúrich

La estación está integrada dentro de la red de trenes de cercanías S-Bahn Zúrich, y en la que efectúan parada los trenes de varias líneas pertenecientes a S-Bahn Zúrich:

Referencias

Weinfelden


Bay Area residents had a rare opportunity Sunday to hear a man who may be the single most influential Muslim in America. But the limits of his reach were also on display.
When Imam W. Deen Mohammed stepped to the podium at the Masonic Auditorium in San Francisco, there were perhaps 300 people in the audience, almost all of them African American.
Though most of his hourlong talk was not about race, the issue that made him a revolutionary in American religion, he didn't shy away from it. He urged audience members to think of themselves not in racial categories but in human terms.
Mohammed spoke of how the Rev. Martin Luther King Jr. dreamed of a day when his children would not be judged by the color of their skin, but the content of their character. But after King's death, Mohammed said black leaders chose another direction.
"Now how come after he died, our leaders talked nothing but 'black' to us," he said. Mohammed said the use of the adjective "black" to describe the community's achievements degraded them - and insulted others.
Noting that African American leaders in Congress refer to themselves as the Congressional Black Caucus, Mohammed questioned how people would react if there was a "white caucus." Mohammed urged those gathered to think about the universality of all people - and that defining religion for any one race is dangerous.
"Black theology weakens our ability to gain from scripture, guidance from scripture, to make ourselves a better religious community," he said.
The words are dramatic considering the path that Mohammed has taken.
Mohammed is the son of Elijah Muhammad, who for more than 30 years led the Nation of Islam, the black separatist religion that deemed all white people to be "devils" and black people to be "gods." W. Deen Mohammed was chosen by his father to carry on his legacy.
But after Elijah Muhammad died in 1975, the son chose a different path. He gradually dissolved the Nation of Islam, leading believers toward the Sunni branch of Islam. All people were equal, regardless of race. Women were the same as men, except for physical strength.
While his father's Nation of Islam explicitly referred to the U.S. flag as a symbol of "slavery, suffering and death," Mohammed started New World Patriotism Day in 1979, according to Imam Faheem Shuaibe, who leads Masjidul Waritheen, an Oakland mosque.


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During the process of your loan, there are certain "Dos and Don'ts" which may affect the outcome of your loan request. Many times credit, income and assets are re-verified after closing.
So, these guidelines remain in effect until your loan has been closed, funded and been recorded.
– Take on any additional debt on your existing credit cards or lines of credit. All debt must be disclosed.
– Change jobs unless it is the same line of work and for equal or higher pay. Please notify us if this occurs.
– Allow anyone to make an inquiry on your credit report.
– Change bank accounts or transfer money within your existing bank accounts.
– Co-sign for anyone on anything.
– Purchase a vehicle or any other real estate.
– Start any home improvements that are not a condition of the loan.
– Keep all accounts current; mortgages, car payments, credit cards, utilities, etc.
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text:
Noshin Hoque, Policy Coordinator
August 03, 2021 by Rise
Noshin Hoque is a political-social worker and social justice advocate. She recently graduated with her MSW, specializing in policy practice, from Columbia University. Noshin is passionate about environmental justice, educational equality, immigration rights — and most importantly, envisioning alternatives to current oppressive systems. Noshin worked with the Congressional Research Institute for Social Work and Policy, Legislators at the Suffolk County Legislature, and the Action Lab for Social Justice throughout her professional career. She was also a member of the NASW-NYS PACE committee, where she endorsed over 20 candidates running for elected office.
At Rise, Noshin hopes to build connections with communities and advocate for social issues through policy and structural change. As policy coordinator, she assists with relationship- and coalition-building to support legislative and budget advocacy at the city and state levels. Her work supports Rise's shift to community organizing to reverse NYC's reliance on harmful family policing systems and under-investment in communities.
Noshin@risemagazine.org


Four fine art photographs featuring the amazing waves of the ocean. This set of four beach decor prints are finished in pale blue, tan and taupe tones.
Absolutely beautiful photos! I only wish I had gotten the bigger size. They are stunning pictures, were packaged well and came quickly. All around wonderful experience!
I love this photographs, they arrived very quickly and they look great.
It's so cute perfect for my nursery! Definitely more of an aqua than it looked in the pic (at least on my computer) but I like it better that way so I'm happy.
Ordered this set of prints for our bathroom - they are lovely! Came so fast and can't wait to frame and get them up, thanks!
Just AMAZING art work!!!! Lisa was so wonderful to work with too.


text:
About Touchpoints
Exploring the power of packaging to engage consumers
New compostable packaging solution for loose tea brand
Parkside has collaborated with SUKI Tea to develop a printed pack for its various loose tea products, replacing a plain design. The company says that this is a step further towards its sustainability goals to be 100% plastic free by 2022.
Made from bio-based materials and featuring a compostable zipper, the new pouch design provides excellent oxygen, aroma and moisture barrier that extend the shelf life of the tea while maintaining optimum flavour.
Zoë McCullough, Sales and Marketing Manager at SUKI, said: "Customers are becoming increasingly aware of their environmental impact and therefore eco-friendly packaging was a key for SUKI. It's been a challenge but an important one that links closely to our core ethics and ethos, Parkside have been instrumental in achieving one of key objectives – Plastic-free tea packaging.
"Favouring ethical supplier practices and operating in a more socially, economically and environmentally sustainable manner are the cornerstones of everything we do so it was a natural next step for SUKI. Working with Parkside has been great, matching our values in and delivering outstanding compostable packaging."
Suitable for industrial composting
The SUKI Tea packaging adds to the portfolio of Park2NatureTM compostable packaging solutions Parkside currently provides. The packs are designed to break down within 26 weeks, as well as suitable for industrial composting facilities and complies with A Plastic Planet's Plastic Free Trust Mark. The high definition graphics created with HD compostable inks also can provide greater shelf appeal for the tea brand.
Paula Birch, Sales & Innovations Director at Parkside, said: "Suki Tea is an adventurous, responsible brand that respects and values people and the planet. Working with the team was a privilege and we are extremely pleased we were able to help the brand to achieve an innovative pack solution that is sustainable in every way."
Editor of Touchpoints magazine, writer for Packaging Europe magazine and design enthusiast!
editor@packtouchpoints.com
Cadbury celebrates new global brand identity
Capturing the essence of a new gin blend
Beer hues through Pantone
Subscribe to Touchpoints
The first edition of Touchpoints magazine is set to hit desks in early April. You can make sure to be one of the first recipients of this brand-new magazine by subscribing here!
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text:
\section{Introduction}\label{sec:intro}

Photon-hadron production in high energy $pp$ and $pA$ collisions has been put forward \cite{Jalilian-Marian:2005qbq,Jalilian-Marian:2008jjn} as a promising probe of the small-$x$ hadron wavefunction \cite{Iancu:2003xm,Jalilian-Marian:2005ccm,Gelis:2010nm}. The distinguished character of this process lies in the fact that a well isolated photon does not participate in strong interactions and therefore the uncertainties related to hadronization of the final state are reduced compared to the more abundant di-hadron ($hh$) production.
The isolated photon component is defined to be separated by a suitable isolation algorithm from the so-called \emph{decay photons}, which are radiated from the $\pi^0 \to \gamma\gamma$ decays. This, in turn, suppresses photons fragmenting off jets in the course of hadronization. Recently, the PHENIX collaboration at RHIC \cite{PHENIX:2016zxb,PHENIX:2018trr} and the ALICE collaboration at the LHC \cite{Acharya:2020sxs} reported on the measurements of the cross section of an isolated photon in association with an unidentified charged hadron in $pp$ and $pA$ that is within the kinematic region potentially sensitive to small-$x$ physics. In this work we are motivated to pursue the phenomenological implications of those measurements for the first time.

A long standing hypothesis in high energy QCD is that the rapid growth of gluon radiation inside the hadron wavefunction at small-$x$ is balanced out by a gluon recombination process, which leads to the phenomena of gluon saturation. The theoretical framework behind this basic picture is called the Color Glass Condensate (CGC) \cite{Iancu:2003xm,Jalilian-Marian:2005ccm,Gelis:2010nm} where the energy, or small-$x$, enhanced logarithms $\sim \alpha_S \log (s) \sim \alpha_S\log \left(1/x\right)$, can be consistently resummed at each order in the strong coupling $\alpha_S$. The resulting gluon radiation in CGC becomes concentrated around a dynamically generated transverse momentum - the saturation scale $Q_S$, that is build up from multiple scattering of partons on the dense target.  In the context of the simultaneous production of two particles, the back-to-back transverse momenta kinematics of the conventional leading order $2\to 2$ partonic process gets disrupted in the CGC. This becomes more dramatic for a heavy nuclei, where a scaling $Q_S^2 \sim A^{1/3}$ is expected.

It is with the above picture in mind that $\gamma h$ \cite{Jalilian-Marian:2012wwi,Rezaeian:2012wa,Rezaeian:2016szi,Benic:2017znu,Goncalves:2020tvh} and $\gamma^* h$ \cite{Stasto:2012ru,Basso:2015pba,Basso:2016ulb} production in $pA$ (and recently also the related $\gamma-{\rm jet}$ production in $eA$ \cite{Kolbe:2020tlq}) have been explored as possible pathways to a phenomenological validation of the CGC. Saturation effects become prominent when the imbalance momenta of the photon ($\kgp$) and the underlying final state parton ($\boldsymbol{q}_\perp$) is of the order of the saturation scale $k_\perp \equiv |\kgp + \boldsymbol{q}_\perp| \sim Q_S$. In terms of the distribution over the azimuthal angle $\Delta\phi \equiv \phi_\gamma - \phi_h$, the general expected feature is a broadening of the away side peak, $\Delta \phi = \pi$, as the kinematics condition $k_\perp \to Q_S$ becomes satisfied.

While both $\gamma h$ and $hh$ production are understandable with such a simple physics argument of the broadening of the away side peak, further investigation into the two processes revealed that they are sensitive to two different unintegrated gluon distributions (UGD)s \cite{Kharzeev:2003wz}. At leading order, $\gamma h$ production is probing the gluon dipole distribution, while $hh$ production is instead probing a combination of the dipole and the Weisz\" acker-Williams distribution \cite{Dominguez:2010xd,Dominguez:2011wm}. These two UGDs have a completely different behavior at small $k_\perp$ (see e.~g. \cite{Dominguez:2011wm} and also Eq.~\eqref{eq:dpww} in the following section). Thus, according to CGC, the theoretical prediction for $\gamma h$ production at the away side peak may look nothing like the prediction for $hh$ production. Indeed this is another reason to explore $\gamma h$ production in CGC.

Alternatively, the broadening of the away side peak may
be completely unrelated to the initial state, but simply be induced by the soft gluon radiation, the so-called Sudakov effect \cite{Sudakov:1954sw,Dokshitzer:1978hw,Parisi:1979se,Collins:1984kg,Collins:2011zzd}. Soft gluon radiation generates double logs as $\alpha_S\log^2(k_\perp/Q)$, where $Q$ is a hard scale in the process, and therefore becomes enhanced when the underlying individual partonic transverse momenta is hard, $k_\perp \ll Q$. For the high energy kinematics case when in addition $k_\perp \sim Q_S$ holds, saturation effects and Sudakov effects become two contributing mechanisms and so clearly both should be taken into account. A recent development \cite{Mueller:2012uf,Mueller:2013wwa} showed that it is possible to perform a simultaneous resummation of both the Sudakov logs and the small-$x$ logs in a consistent way. On the other hand, since $Q_S^2 \sim A^{1/3}$ for a heavy nuclei, it is expected the saturation effect would become more important in the $pA$ collision, while both saturation and Sudakov effect are needed for a proper description in $pp$ collisions. This is indeed confirmed by recent studies in $hh$ production \cite{Stasto:2018rci,vanHameren:2020rqt} but also in dijet \cite{vanHameren:2019ysa}, $Z$-boson \cite{Marquet:2019ltn} and $Z$-jet \cite{vanHameren:2015uia} productions as well as in related processes in $eA$ collisions \cite{Zheng:2014vka,Zhao:2021kae,vanHameren:2021sqc}, which prompts us to take into account both the small-$x$ and Sudakov effects in order to establish a realistic baseline for a proper extraction of the appropriate nuclear modifications based on a comparison of the obtained results in $pp$ and $pA$ collisions.

The main purpose of this work is to perform a numerical computation of the isolated photon-hadron cross section within the CGC framework, while taking into account Sudakov effects for the first time. In Sec.~\ref{sec:framework} we explain our approach with the main formulas given in \eqref{eq:W} and \eqref{eq:incgammahlo2}. Our numerical results, shown in Sec.~\ref{sec:results}, concern the azimuthal angle ($\Delta \phi$) distributions measured at RHIC at 200 GeV and 510 GeV in $pp$ and the LHC at 5.02 TeV in $pp$ and $p$Pb and also the out-of-plane transverse momentum distributions measured at RHIC. Our main finding is that while the CGC results alone produce too narrow distributions compared to the data a reasonable agreement with the data is possible when the Sudakov effect is taken into account. Additionally we provide predictions for the magnitude of the nuclear effect in $pA$ vs $pp$ also arguing in favour of more symmetric transverse momentum kinematics of the $\gamma h$ system where the effect of gluon saturation would be better resolved. In the final Section~\ref{sec:conc} we summarize our findings while also providing an outlook to further theoretical investigations.

\section{Theoretical framework}
\label{sec:framework}

In this section we give a quick recap of the main formulas that will be used in obtaining our numerical results for $p (P_p) A (P_A) \to h^{\pm} (P_h)\gamma (k_\gamma) X$ production. Throughout this work, we will use  $p$ for the projectile proton, $A$ for the target nucleus (or proton in $pp$ collisions). We will also use the shorthand notation $h^\pm \equiv h^+ + h^-$ to express observables which are obtained by adding the contributions of positive and negative unidentified charged hadrons. We will be using the leading order formulas for $\gamma h$ production - at mid-rapidity the dominant channel is $q(p)g(k) \to q(q) \gamma(k_\gamma)$, which we firstly address below in the CGC framework, and subsequently incorporate soft gluon resummation in the following subsection. The final formula that we will be using in our numerical computations is given in \eqref{eq:W} and \eqref{eq:incgammahlo2}.

\subsection{Photon-hadron cross section in the CGC framework}\label{sec:phXsec}

The following CGC formulas are computed using a dilute-dense framework \cite{Iancu:2003xm,Jalilian-Marian:2005ccm,Gelis:2010nm} where a dilute projectile parton passes through a dense (nuclear) target described by a classical gluon field. In the dilute-dense framework an all-order scattering on the target is taken into account building up a finite transverse momentum in the final state, while the dilute projectile is treated order-by-order in perturbation theory.
The leading order $pA\to h\gamma X$ inclusive CGC cross section
can be straightforwardly obtained from the underlying partonic $q g \to q\gamma$ \cite{Kopeliovich:1998nw,Gelis:2002ki,Baier:2004tj} channel.
In the massless quark limit it simplifies
to the following expression,
\begin{equation}
\frac{\mathrm{d} \sigma}{\mathrm{d}^2 \kgp \mathrm{d} \eta_\gamma\mathrm{d}^2 \boldsymbol{P}_{h\perp}\mathrm{d} \eta_h} = (\pi R_A^2) \sum_q\int_0^1 \frac{\mathrm{d} z_h}{z_h^2} D_q(z_h,\mu^2)\frac{e_q^2 N_c}{8\pi^4} x_p f_q(x_p,\mu^2)\boldsymbol{k}_\perp^2\tilde{\mathcal{N}}_{A,Y_A}(\boldsymbol{k}_\perp)\hat{\sigma}\,,
\label{eq:incgammahlo}
\end{equation}
where $f_q(x_p,\mu^2)$ is the collinear quark distribution function, $D_q(z_h,\mu^2)$ is the relevant collinear fragmentation function of a quark with flavor $q$ and momenta $q^\mu = P_h^\mu/z_h$ to a particular hadron species at a factorization scale $\mu^2$. In this work we are using the CTEQ6M quark distributions \cite{Pumplin:2002vw} and the DSS fragmentation functions \cite{deFlorian:2007aj}.

We have $\boldsymbol{k}_\perp \equiv \kgp + \boldsymbol{q}_\perp$ as the imbalance momentum. Furthermore, $(\pi R_A^2)$ is the target area. The hard factor $\hat\sigma$ is given as
\begin{equation}
\hat{\sigma} = \frac{\alpha_e}{2 N_c}\frac{P_{q\gamma}(z)}{q\cdot k_\gamma} \frac{z^2}{\kgp^2}\quad \text{with} \quad P_{q\gamma}(z) = \frac{1 + (1-z)^2}{z}\,.
\end{equation}
Here,  $P_{q\gamma}(z)$ is the quark-to-photon splitting function with $z = k_\gamma^+/(k_\gamma^+ + q^+)$. The remaining kinematic variables are given as
\begin{equation}
x_p = \frac{k_\gamma^+ + q^+}{P_p^+} \,, \qquad x_A= \frac{k_\gamma^- + q^-}{P_A^-}\,, \qquad Y_A = \log \frac{1}{x_A}\,,
\label{eq:kin}
\end{equation}
with the projectile and target light-cone momenta in the center of mass frame given as $P_A^- = P_p^+ = \sqrt{\frac{s}{2}}$, where $s$ is the center-of-mass collision energy. Here, and in the following, the light-cone variables are defined as $p^{\pm} = (p^0 \pm p^3)/\sqrt{2}$ with the rapidity $\eta = \log(p^+/p^-)/2$. $\eta_\gamma$ and $\eta_h$ are the photon and the hadron rapidities, respectively.

The function $\tilde{\mathcal{N}}_{A,Y_A}(\boldsymbol{k}_\perp)$ is the CGC dipole in the fundamental representation
\begin{equation}
\tilde{\mathcal{N}}_{A,Y_A}(\boldsymbol{k}_\perp) = \int \mathrm{d}^2 \bperp \mathrm{e}^{\mathrm{i}\boldsymbol{k}_\perp\cdot \bperp} \tilde{\mathcal{N}}_{A,Y_A}(\bperp)\,, \qquad  \tilde{\mathcal{N}}_{A,Y_A}(\bperp) = \frac{1}{N_c} {\rm tr}_c \langle \tilde{U}(\bperp) \tilde{U}^\dag(0) \rangle_{Y_A}\,,
\label{eq:dip}
\end{equation}
where $\tilde{U}(\bperp)$ is the fundamental light-like Wilson line arising from all order scattering on the dense target. The $k_\perp$-dependent gluon distribution $\varphi_{\rm DP}(Y,\boldsymbol{k}_\perp)\sim \boldsymbol{k}_\perp^2\tilde{\mathcal{N}}_{Y}(\boldsymbol{k}_\perp)$ in \eqref{eq:incgammahlo}, signifies a broadening of the collinear $2\to 2$ away side peak, that would be represented simply by a $\delta^{(2)}(\boldsymbol{k}_\perp)$ (see \eqref{eq:pqcd}) and that is also shifted from $k_\perp = 0$ to $k_\perp \sim Q_S$.

As mentioned in the introduction, a well known theoretical distinction of $\gamma h$ with respect to $hh$ correlations is that they probe fundamentally different gluon distributions \cite{Dominguez:2010xd,Dominguez:2011wm}. The leading order $\gamma h$ cross section is proportional to the gluon dipole distribution $\varphi_{\rm DP}(Y,\boldsymbol{k}_\perp)$, while the leading order $hh$ cross section is proportional to a combination of the Weisz\" acker-Williams gluon distribution $\varphi_{\rm WW}(Y,\boldsymbol{k}_\perp)$ and the dipole distribution \cite{Dominguez:2010xd,Dominguez:2011wm}. While these two distributions both display a high-$k_\perp$ perturbative $1/\boldsymbol{k}_\perp^2$ tail, their behavior is completely different for low $k_\perp$ where we have
\begin{equation}
\varphi_{\rm DP}(Y,\boldsymbol{k}_\perp)\sim \boldsymbol{k}_\perp^2/Q_S^2\,, \qquad \varphi_{\rm WW}(Y,\boldsymbol{k}_\perp)\sim \log(Q_S^2/\boldsymbol{k}_\perp^2)\,.
\label{eq:dpww}
\end{equation}
This prediction is particularly important at the away-side-peak, $\Delta\phi = \pi$, where small values of $k_\perp$ would be probed. In the case of $\gamma h$ correlations, $\varphi_{\rm DP}(Y,\boldsymbol{k}_\perp)$ causes a dip in the cross section, see \cite{Rezaeian:2012wa} and also \cite{Rezaeian:2016szi,Goncalves:2020tvh,Stasto:2012ru,Basso:2015pba,Basso:2016ulb}, since the underlying partonic cross section in \eqref{eq:incgammahlo} is strictly vanishing as the kinematics condition $k_{\perp} = |\kgp + \boldsymbol{q}_\perp|$ becomes satisfied. On the other hand, due to the low $k_\perp$ behavior of $\varphi_{\rm WW}(Y,\boldsymbol{k}_\perp)$ the $hh$ production would rather level off to a constant at the away side peak.

In this paper, the $Y_A$ dependence of the gluon dipole follows the running coupling Balitsky-Kovchegov evolution equation \cite{Balitsky:1995ub,Kovchegov:1999yj,Balitsky:2006wa} (rcBK) which is a good approximation to the more general Jalilian-Marian-Iancu-McLerran-Weigert-Leonidov-Kovner (JIMWLK) evolution \cite{JalilianMarian:1997jx,JalilianMarian:1997dw,Iancu:2000hn,Iancu:2001ad} of the dipoles. As a general feature of small-$x$ evolution the distribution broadens as $x$ becomes smaller. The initial condition for the rcBK evolution is set at $x = x_0 = 0.01$ where the dipole is given by the anomalous dimension McLerran-Venugopalan (MV) model,  which we will call here the MV$^\gamma$ model. The initial condition for the rcBK evolution of the fundamental dipole is explicitly given by
\begin{equation}
\tilde{\mathcal{N}}_{Y_0}(\xp) = \exp\left\{- \frac{\left(x_\perp^2 Q_{S0}^2\right)^{\gamma}}{4} \log\left(\frac{1}{x_\perp \Lambda_{\rm IR}}+ \mathrm{e}\right)\right\}\,,
\end{equation}
where $Y_0 = \log 1/x_0$, $Q_{S0}$ is the initial saturation momentum, $\gamma$ is the anomalous dimension and $\Lambda_{\rm IR}$ is the IR cutoff of the model. We use the parameter set \cite{Albacete:2010sy} $\gamma = 1.119$, $(Q_{S,0}^p)^2 = 0.169 \, {\rm GeV}^2$, $\Lambda_{\rm IR} = 0.241 \, {\rm GeV}$. The rcBK equation provides the dipole distribution at $x < x_0$ while for $x > x_0$ we use the matching to the collinear gluon PDF as explained in \cite{Ma:2015sia}. The matching procedure fixes the proton radius to $R_p = 0.5257$ fm. For the nuclei we use $Q_{S0,A}^2 = c A^{1/3} Q^2_{S0,p}$ where $c\simeq 0.5$ \cite{Dusling:2009ni}. In our computations we set $Q_{S0,A}^2 = 3 Q^2_{S0,p}$ for heavy nuclei such as Pb and Au.

We will be computing the cross section for an isolated $\gamma h$ production, defined in a standard way through a fixed isolation cut in $\eta-\phi$ space around the photon, defined by $(\eta_\gamma,\phi_\gamma)$. An isolation cone, $R$, is introduced to cut out a region where $\sqrt{\Delta \eta^2 + \Delta\phi^2} < R$ in order to isolate the photon from any soft and collinear hadronic activity within $R$. Here $\Delta \eta = \eta_\gamma - \eta_h$ and $\Delta\phi = \phi_\gamma - \phi_h$. For the cross section at hand \eqref{eq:incgammahlo} this effectively suppresses its fragmentation component that would appear when $\gamma$ is being emitted collinearly to the underlying final state parton \cite{Jalilian-Marian:2012wwi}.

\subsection{Implementing the Sudakov effect}
\label{sec:sudakov}

The implementation of the Sudakov effect rests on the Collins-Soper-Sterman (CSS) or transverse momentum resummation formalism \cite{Collins:1984kg,Collins:2011zzd}. The inclusion of soft gluon radiation to all orders introduces a transverse momentum dependence into the distribution and fragmentation functions that follows the CSS evolution equation \cite{Collins:1984kg,Collins:2011zzd}. The result of CSS evolution is obtained in $\bperp$-space resulting in a compact formula for the so-called Sudakov factor. Refs.~\cite{Mueller:2012uf,Mueller:2013wwa} further demonstrated that Sudakov resummation can be accomplished on top of the small-$x$ resummation at the one-loop order. In the context of $\gamma h$ production considered here the relevant part of the cross section \eqref{eq:incgammahlo} gets modified through
\begin{equation}
\boldsymbol{k}_\perp^2 \tilde{\mathcal{N}}_{A,Y_A}(\boldsymbol{k}_\perp) D_q(z_h,\mu^2) f_q(x_p,\mu^2) \to \int \mathrm{d}^2 \bperp \mathrm{e}^{\mathrm{i}\boldsymbol{k}_\perp\cdot \bperp} \partial^2_{\bperp}\tilde{\mathcal{N}}_{A,Y_A}(\bperp)D_q(z_h,\mu_b^2) f_q(x_p,\mu_b^2)\, \mathrm{e}^{-S_{\rm Sud}(\bperp,Q)}\,,
\label{eq:sud1}
\end{equation}
where we multiplied by a prefactor $\boldsymbol{k}_\perp^2$ to get the unintegrated gluon distribution\footnote{See Appendix \ref{sec:appa} for the corresponding collinear formula.}. In Eq.~\eqref{eq:sud1} the exponential $e^{-S_{\rm Sud}(\bperp,Q)}$ corresponds to the resummed contribution from soft-gluon radiations,
where the Sudakov factor $S_{\rm Sud}(\bperp,Q)$,  has been introduced as the radiation kernel summed over $\mu_b$ up to the hard scale $Q$. The Sudakov factor is given by the following generic form \cite{Sun:2014gfa,Sun:2015doa}
\begin{equation}
S_{\rm Sud}(\bperp,Q) = \int_{\mu_b^2}^{Q^2} \frac{d\bar{\mu}^2}{\bar{\mu}^2} \left[A \log\left(\frac{Q^2}{\bar{\mu}^2}\right) + B\right]\,,
\label{eq:sudpertcgc}
\end{equation}
Here $\mu_b$ is a factorization scale according to the $b_*$-prescription \cite{Collins:1984kg}
\begin{equation}
\mu_b  = \frac{2 \mathrm{e}^{-\gamma_E}}{b_*} \,, \qquad b_*^2 = \frac{\bperp^2}{1 + \frac{\bperp^2}{b_{\rm max}^2}}\,,
\end{equation}
where $b_{\rm max} = 1.5$ GeV$^{-1}$. With this prescription $\mu_b > 2 \mathrm{e}^{-\gamma_E}/b_{\rm max}$ thus preventing the $\bperp$-integral from entering the non-perturbative region. For the hard scale we take $Q^2  = x_p x_A s$. The quantities $A$ and $B$ are channel dependent coefficients that can be computed in perturbation theory. For each initial and final state quark (or gluon) in the channel we have $A_q = \alpha_S C_F/(2\pi)$, $A_g = \alpha_S C_A/(2\pi)$, and
$B_q = -\alpha_S \frac{3}{2}C_F/(2\pi)$, $B_g = -\alpha_S 2C_A \beta_0/(2\pi)$, where $\beta_0 =\left(11 - \frac{2 N_f}{3}\right)/12$ at one-loop order \cite{Sun:2014gfa,Sun:2015doa}.
According to Refs. \cite{Mueller:2012uf,Mueller:2013wwa},  the pertubative prefactor is absent in the single-log $B$ term for the case of any incoming small-$x$ gluon.  Consequently, we do not count the small-$x$ gluon in obtaining this coefficient. For the $qg \to q \gamma$ channel we should use
\begin{equation}
A = 2A_q + A_g = \frac{\alpha_S(\bar{\mu}^2)}{\pi}\left( C_F + \frac{C_A}{2}\right)\,, \qquad B = 2 B_q = - \frac{\alpha_S(\bar{\mu}^2)}{\pi} \frac{3}{2} C_F\,.
\label{eq:absud}
\end{equation}

In order to compensate for the missing effect at large $\bperp$ it is common to add a non-perturbative Sudakov factor $S_{\rm non-pert}(\bperp,Q)$ as
\begin{equation}
S_{\rm Sud}(\bperp,Q) \to S_{\rm Sud}(\bperp,Q) + S_{\rm non-pert}(\bperp,Q)\,.
\end{equation}
In this work we are using the parametrization \cite{Sun:2014dqm}
\begin{equation}
S^q_{\rm non-pert}(\bperp,Q) = \frac{g_1}{2}\bperp^2 + \frac{1}{4}\frac{g_2}{2}\log\frac{Q^2}{Q^2_0}\log\frac{\bperp^2}{b_*^2}\,, \qquad S^g_{\rm non-pert}(\bperp,Q) = \frac{C_A}{C_F}S^q_{\rm non-pert}(\bperp,Q)\,,
\label{eq:sudnonpert}
\end{equation}
where $g_1 = 0.212$ GeV$^2$, $g_2 = 0.84$, $Q_0^2 = 2.4$ GeV$^2$. Eq.~\eqref{eq:sudnonpert} should in principle be used for each quark and gluon in the initial or the final state.  The small-$x$ gluon already contains some non-perturbative information through the $k_\perp$-dependent distribution.
To avoid any possible double counting, the small-$x$ gluon is therefore dropped \cite{Zheng:2014vka,Stasto:2018rci} and we have
$S_{\rm non-pert}(\bperp,Q) = 2 S^q_{\rm non-pert}(\bperp,Q)$.

Denoting
\begin{equation}
W(z_h,x_p,\bperp,Q) \equiv \sum_q \frac{e_q^2 N_c}{8\pi^4} D_q(z_h,\mu_b^2)f_q(x_p,\mu_b^2)\mathrm{e}^{-S_{\rm Sud}(\bperp,Q)-S_{\rm non-pert}(\bperp,Q)}\,,
\label{eq:W}
\end{equation}
our final formula for the $\gamma h$ cross section reads
\begin{equation}
\frac{\mathrm{d} \sigma}{\mathrm{d}^2 \kgp \mathrm{d} \eta_\gamma\mathrm{d}^2 \boldsymbol{P}_{h\perp}\mathrm{d} \eta_h} = (\pi R_A^2) \int_0^1 \frac{\mathrm{d} z_h}{z_h^2} \int\frac{\mathrm{d}^2 \boldsymbol{k}_\perp'}{(2\pi)^2}W(z_h,x_p,\boldsymbol{k}_\perp' - \boldsymbol{k}_\perp,Q) \boldsymbol{k}_\perp'^2\tilde{\mathcal{N}}_{A,Y_A}(\boldsymbol{k}_\perp')\hat{\sigma}\,,
\label{eq:incgammahlo2}
\end{equation}
where we recall that $\boldsymbol{k}_\perp = \kgp + \boldsymbol{P}_{h\perp}/z_h$.
The explicit computation of Eq.~\eqref{eq:incgammahlo2} is performed in momentum space through a convolution of the momentum space gluon distribution, $\boldsymbol{k}_\perp^2 \tilde{\mathcal{N}}_{A,Y_A}(\boldsymbol{k}_\perp)$,  with the Fourier transform of $W(z_h,x_p,\bperp,Q)$. The latter is computed numerically with the algorithm in \cite{Kang:2019ctl}. We also remark that with resumming infinite number of soft gluons exact kinematics relations \eqref{eq:kin} are lost, and in practice \cite{Mueller:2016gko,Chen:2016vem} one resorts to an approximate relation $x_{p,A} = p_\perp (\mathrm{e}^{\pm\eta_\gamma} + \mathrm{e}^{\pm\eta_h})/\sqrt{s}$, with $p_\perp \equiv {\rm max}(k_{\gamma\perp},q_\perp)$.

According to \eqref{eq:W} the Sudakov factor brings an additional dependence of the imbalance $k_\perp$-distributions on the hard scale $Q$. As a typical result of CSS evolution, the $k_\perp$ distribution gets broadened as a function of the hard scale $Q$. This can be intuitively understood from the leading $\log^2(k_\perp^2/Q^2)$-dependence as the increase in the hard scale brings more opportunity for soft gluon radiation. In the CGC framework radiative processes are enhanced as $\log(1/x)$. Therefore, since $x \sim Q/\sqrt{s}$, an increase in the hard scale would lead to a narrower distribution. It is thus theoretically and phenomenologically interesting to check the interplay between the small-$x$ resummation and the Sudakov resummation.

\section{Numerical results and discussion}
\label{sec:results}

\begin{figure}
  \begin{center}
  \includegraphics[scale = 0.5]{phenix_200gev.pdf}
  \end{center}
  \caption{Isolated $\gamma h^{\pm}$ angular distribution for mid-rapidity $pp$ collisions at $200$ GeV given in $k_{\gamma\perp}\times P_{h\perp}$ bins vs data from PHENIX \cite{PHENIX:2018trr}. The experimental data has been shifted for the underlying event. The solid magenta line corresponds to the combined CGC w Sud calculation, while the CGC w/o Sud and Sud computations correspond to the thin orange and dashed teal lines, respectively.}
  \label{fig:cpphenix200}
\end{figure}

In this Section we perform
a numerical computation of the cross section for the isolated $\gamma h$ cross section based on \eqref{eq:incgammahlo2}. In what follows,  we abbreviate this result as as CGC w(ith) Sud(akov). To isolate the effects of both small-$x$ and Sudakov gluons and to gain further insight we will also show results from the CGC framework alone (Eq. \eqref{eq:incgammahlo}),  and from the cross-section in the collinear pQCD framework with only the Sudakov effect taken on account. For the latter we refer to \eqref{eq:colsud} in Appendix \ref{sec:appa}. We abbreviate these results as CGC w/o Sud and Sud, respectively.

To keep the discussion within phenomenological reach, we will mostly study systems and kinematic windows already probed by different experimental collaborations.  Firstly,  the PHENIX experiment measured isolated $\gamma h^\pm$ production in $pp$ collisions at $\sqrt{s} = 200$ GeV \cite{PHENIX:2018trr}, covering the kinematic range
\begin{equation}
|\eta_\gamma| < 0.35 \,, \qquad 5 \, {\rm GeV} < k_{\gamma\perp} < 15 \, {\rm GeV} \,, \qquad |\eta_h| < 0.35 \,, \qquad 0.5 \, {\rm GeV} < P_{h\perp} < 10 \, {\rm GeV}\,,
\label{eq:phenix200}
\end{equation}
where an isolation cut $R = 0.3$ has been applied to the photon. For $\sqrt{s} = 510$ GeV collisions \cite{PHENIX:2016zxb} we have the following kinematics
\begin{equation}
|\eta_\gamma| < 0.35 \,, \qquad 7 \, {\rm GeV} < k_{\gamma\perp} < 15 \, {\rm GeV} \,, \qquad |\eta_h| < 0.35 \,, \qquad 0.7 \, {\rm GeV} < P_{h\perp} < 10 \, {\rm GeV}\,,
\label{eq:phenix510}
\end{equation}
and $R = 0.4$. The kinematics \eqref{eq:phenix200} and \eqref{eq:phenix510} has been further separated in $k_{\gamma\perp} \times P_{h\perp}$ bins as indicated in Figs.~\ref{fig:cpphenix200} and \ref{fig:cpphenix510}, respectively.

The ALICE experiment measured isolated $\gamma h^{\pm}$ production in $pp$ and $p$Pb collisions at $\sqrt{s} = 5.02$ TeV \cite{Acharya:2020sxs} with the following kinematics
\begin{equation}
|\eta_\gamma| < 0.67 \,, \qquad 12 \, {\rm GeV} < k_{\gamma\perp} < 40 \, {\rm GeV} \,, \qquad |\eta_h| < 0.8 \,, \qquad 0.5 \, {\rm GeV} < P_{h\perp} < 10 \, {\rm GeV}\,,
\end{equation}
and $R = 0.4$. The transverse hadron momenta $P_{h\perp}$ is further distributed into bins as indicated in Fig.~\ref{fig:cpalice}.

Before considering the results we make a general remark about our computation based on \eqref{eq:incgammahlo2}. In the kinematics region where the transverse momentum of the final state $\kgp + \boldsymbol{P}_{h\perp}$ is large, and where also $(\kgp + \boldsymbol{P}_{h\perp})^2 \ll Q^2$, the perturbative Sudakov factor, \eqref{eq:sudpertcgc}, would dominate the overall two-particle momentum imbalance in the cross section. While the non-perturbative Sudakov factor is necessary to carry out the $\bperp$-integral, it is irrelevant for the $k_\perp$-spectrum, as demonstrated in \cite{Mueller:2016gko}. However, in our computations this is not completely the case, since for RHIC kinematics we have $Q \sim 7-21$ GeV, where the non-perturbative Sudakov factor should also play a role. At the LHC $Q \sim 17-55$ GeV, but also $k_\perp$ is possibly larger due to the more asymmetric $\gamma h$ momenta configuration.

We will first show our results for the angular distributions and compare them with the data from RHIC and the LHC. In our compuations we focus only on the shape of the $\gamma h$ yield and thus normalize both our theoretical curves and the experimental data to unity. Similar procedure has been employed e.~g. in \cite{Chen:2016vem,Chen:2018fqu,Stasto:2018rci}. We compute as well the normalized out-of-plane transverse momentum distributions and extract their Gaussian widths and compare both with the data from RHIC. We also provide the predicted nuclear modifications by showing the CGC w Sud computation at RHIC and the LHC.

\subsection{Angular distributions}

\begin{figure}
  \begin{center}
  \includegraphics[scale = 0.4]{phenix_510gev_cropped.pdf}
  \end{center}
  \caption{Isolated $\gamma h^{\pm}$ angular distribution for mid-rapidity $pp$ collisions at $510$ GeV given in $k_{\gamma\perp}\times P_{h\perp}$ bins vs data from PHENIX \cite{PHENIX:2016zxb}. The experimental data has been shifted for the underlying event.}
  \label{fig:cpphenix510}
\end{figure}

In Fig.~\ref{fig:cpphenix200} we compare our CGC w Sud result with the $200$ GeV $pp$ data at RHIC \cite{PHENIX:2018trr} and find a fair agreement in most of the bins. Here the experimental data have been shifted vertically for the underlying event, that is, by the background of uncorrelated $\gamma h^\pm$ pairs \cite{PHENIX:2018trr}. The CGC w Sud results are also compared with a CGC w/o Sud computation. The away side peak from the CGC w/o Sud results is clearly too narrow to be able to describe the data. As argued previously, the dip at $\Delta \phi = \pi$, and the resulting double peak structure around it, for the CGC w/o Sud computation is due to the low $k_\perp$ behavior of the dipole gluon distribution $\varphi_{\rm DP}(Y,\boldsymbol{k}_\perp) \sim \boldsymbol{k}_\perp^2 /Q_S^2$. For this kinematics the double peak is strongly focused in a narrow region around $\Delta \phi = \pi$. Let us stress again here that the presence of a double peak in general is a robust prediction \cite{Rezaeian:2012wa,Rezaeian:2016szi,Goncalves:2020tvh,Stasto:2012ru,Basso:2015pba,Basso:2016ulb} of the leading order $\gamma h$ production in CGC. From the PHENIX data alone it is difficult to find support for this feature, though it might be simply missed by the experimental resolution. In any case, our prediction is that, for the kinematics considered here, the double peak is completely washed away by including the Sudakov effect. It is instructive to also compare to a Sud only result based on the leading order $qg \to q\gamma$ collinear formula. While the Sud result gets closer to the data than CGC w/o Sud in general, best results are obtained when both the CGC and the Sudakov effects are taken into account.

\begin{figure}
  \begin{center}
  \includegraphics[scale = 0.5]{alice_5020gevincl.pdf}
  \end{center}
  \caption{Isolated $\gamma h^{\pm}$ angular distribution for mid-rapidity $pp$ and $p$Pb collisions at $5.02$ TeV for $12 \, {\rm GeV} < k_{\gamma\perp} < 40 \, {\rm GeV} $ for three bins in $P_{h\perp}$ vs data from ALICE \cite{Acharya:2020sxs}. The magenta points (lines) correspond to $pp$ collisions while the teal squares (lines) correspond to a $p$Pb collision.}
  \label{fig:cpalice}
\end{figure}

In Fig.~\ref{fig:cpphenix510} we compare the CGC w Sud computation with the $510$ GeV $pp$ data from RHIC \cite{PHENIX:2016zxb} where again we find overall good agreement with the data. In Fig.~\ref{fig:cpalice} we compare with the $5.02$ TeV $pp$ and $p$Pb data from LHC \cite{Acharya:2020sxs} and find good agreement with both the $pp$ and the $p$Pb data. Due to asymmetric kinematics in Fig.~\ref{fig:cpalice} our results show only a small nuclear effect. Below (see Fig.~\ref{fig:alicepred}) we look at more symmetric configurations.

\begin{figure}
  \begin{center}
  \includegraphics[scale = 0.6]{phenix_200gev_pA_cropped.pdf}
  \end{center}
  \caption{Isolated $\gamma h^{\pm}$ angular distribution for mid-rapidity $pp$ and $pA$ collisions at $200$ GeV. The higher curve (and narrower peak) correspond to the  $5<k_{\gamma\perp}< 7$ GeV bin, while the lower (wider) peak corresponds to a harder photon momentum bin, $12<k_{\gamma\perp}< 15$ GeV.}
  \label{fig:phenix200pred}
\end{figure}

In Fig.~\ref{fig:phenix200pred} we make predictions for $pA$ collisions at $200$ GeV by considering a subset of bins from Fig.~\ref{fig:cpphenix200}. We pick up the smallest and the largest $k_{\gamma\perp}$ bin from Fig.~\ref{fig:cpphenix200} and distribute the results along $P_{h\perp}$ bins. For comparison, we also repeat the $pp$ results from Fig.~\ref{fig:cpphenix200}. It is useful at this point to discuss the systematics across bins. Lets compare two $pp$ (or $pA$) curves corresponding to the smallest and the largest $k_{\gamma\perp}$, for a fixed $P_{h\perp}$. We see that as $k_{\gamma\perp}$ (the transverse momentum of the trigger particle) is increased, the away side peak gets narrower. We can understand this in a intuitive way as follows. At large trigger $k_{\gamma\perp}$ also the momentum imbalance $k_\perp$ eventually increases ($P_{h\perp}$ is held fixed) and so the Sudakov logs become less prominent. Note that for high $k_{\gamma\perp}$-kinematics the details of the non-perturbative Sudakov factor should be negligible. At the same time, nonlinear effects from the CGC also play less of a role as with high trigger $k_{\gamma\perp}$ we are probing the perturbative tail of the gluon transverse momentum distribution. Therefore, we expect the probability for a  high-$k_{\gamma\perp}$ trigger photon to scatter at an angle $\Delta\phi \neq \pi$ to be strongly suppressed, explaining the narrower shape.  Likewise,  for smaller $k_{\gamma\perp}$ the away side peak will get broadened. Our second point concerns the nuclear effect that is visible by a comparison of the full ($pp$) and the dashed ($pA$) curves in Fig.~\ref{fig:phenix200pred}. Due to a larger saturation scale in the nuclei than in the proton target we observe a suppression of the away side peak in $pA$ in comparison to $pp$ for all kinematic bins considered.

\begin{figure}
  \begin{center}
  \includegraphics[scale = 0.4]{alice_5020gev_pA_cropped.pdf}
  \end{center}
  \caption{Isolated $\gamma h^{\pm}$ angular distribution for mid-rapidity $pp$ (solid) and $pA$ (dashed) collisions at $5.02$ TeV. Each $pp$ and $pA$ curve pair corresponds to a different binning of photon momentum. In descending order, the pair correspond to bins of $5<k_{\gamma\perp}< 7$ GeV,  $9<k_{\gamma\perp}< 12$ GeV ,  and $12<k_{\gamma\perp}< 15$ GeV.}
    \label{fig:alicepred}
\end{figure}

In Fig.~\ref{fig:alicepred} we present projections for mid-rapidity $pp$ and $pA$ collisions at the LHC energy of $5.02$ TeV. We keep the associated hadron bins from Fig.~\ref{fig:cpalice} and lower the trigger photon $k_{\gamma\perp}$ in order to reach a more symmetric configuration. The imbalance momentum of the $\gamma h^{\pm}$ system thus approaches the saturation scale at the away side peak leading to a more substantial nuclear effect as can be seen from Fig.~\ref{fig:alicepred}.

\subsection{Out-of-plane transverse momentum distributions}

In addition to the angular distributions, PHENIX also measured \cite{PHENIX:2018trr,PHENIX:2016zxb} the so-called out-of-plane $p_{\rm out}$ distributions where $p_{\rm out} \equiv P_{h\perp}\sin(\Delta\phi)$, binned as a function of $x_E \equiv -\kgp\cdot \boldsymbol{P}_{h\perp}/\kgp^2 = -P_{h\perp}\cos(\Delta\phi)/k_{\gamma\perp}$. A quick computation shows that $p_{\rm out}^2 = z_h^2 \boldsymbol{k}_\perp^2 - \kgp^2 (1-x_E/z_h)^2$ at the leading order. Close to the away side peak $\Delta \phi =  \pi$ we have $x_E \simeq z_h$ and so $p_{\rm out} \simeq z_h k_\perp$.  By binning the result in $x_E$, we can appreciate that the $p_{\rm out}$-distributions serve as a proxy for the intrinsic $k_\perp$ distributions \cite{PHENIX:2018trr,Osborn:2018bwn}.

\begin{figure}
  \begin{center}
  \includegraphics[scale = 0.6]{phenix_200gev_poutdist.pdf}
  \end{center}
  \caption{$p_{\rm out}$ distributions for mid-rapidity $pp$ collisions at $\sqrt{s} = 200$ GeV compared to the data from PHENIX \cite{PHENIX:2018trr} in three $x_E$ bins, $0.1<x_E<0.15$ (left), $0.15<x_E<0.25$ (center), and $0.25<x_E<0.5$ (right).The solid magenta line corresponds to the combined CGC w Sud calculation, while the CGC w/o Sud and Sud computations correspond to the thin orange and dashed teal lines, respectively. }
  \label{fig:poutdist}
\end{figure}

In Fig.~\ref{fig:poutdist} we compare our results with the PHENIX 200 GeV data \cite{PHENIX:2018trr} in $x_E$ bins. The CGC w Sud results show a good agreement with the data in the small to moderate $p_{\rm out}$ region (up to $\sim 1-2$ GeV), and also in the large $p_{\rm out}$ region for the $x_E$ bin $0.1 < x_E < 0.15$. For the remaining two bins, the small to moderate $p_{\rm out}$ region ($p_{\rm out} \sim 1-2$ GeV) is also nicely described by our result, while as $p_{\rm out}$ increases our results tend to overshoot the data. For comparison, the CGC w/o Sud computation is also shown where similar conclusions hold as for the angular distributions: the CGC w/o Sud computation produces a too narrow distribution which cannot be accommodated within the experimental data. In addition, the CGC w/o Sud computation predicts a double peak in the distribution concentrated in a narrow region around $p_{\rm out} = 0$. Again, the present PHENIX data sets alone do not allow us to judge clearly whether this feature is supported or not.
We can only underline the importance of a more complete computation, which includes the Sudakov resummation, where a double peak structure is not present for these kinematics. For completeness we also show the results of a Sud computation which seems to do a good job in the moderate $p_{\rm out}$ region, but tends to undershoot the data for large $p_{\rm out}$.

\begin{figure}
  \begin{center}
  \includegraphics[scale = 0.4]{gwidths_phenix.pdf}
  \end{center}
  \caption{Gaussian widths of the $p_{\rm out}$ distributions as a function of the hard scale $k_{\gamma\perp}$ for mid-rapidity $pp$ collisions. The $pp$ results at $\sqrt{s} = 200$ GeV and $\sqrt{s} = 510$ GeV are compared to the data from PHENIX \cite{PHENIX:2018trr}. The magenta bands correspond to the CGC w Sud computation, while the teal bands correspond to the Sud computation.}
  \label{fig:ktbroad}
\end{figure}

To have a closer look at the small $p_{\rm out}$ region, PHENIX extracted the Gaussian widths of the $p_{\rm out}$-distributions across $0.1 < x_E < 0.5$ from Fig.~\ref{fig:poutdist} by assuming a Gaussian-like shape in the range $-1.1 \, {\rm GeV}<p_{\rm out} < 1.1 \, {\rm GeV}$. The systematic error is estimated by varying this range by $\pm 0.2$ GeV \cite{PHENIX:2018trr}.
Using the same procedure we compute the Gaussian widths of the $p_{\rm out}$ distributions from Fig.~\ref{fig:poutdist}. Our results are shown in Fig.~\ref{fig:ktbroad} as a function of the hard scale $k_{\gamma\perp}$ in comparison to the PHENIX 200 GeV and 510 GeV $pp$ data. The theoretical bands correspond to varying the $p_{\rm out}$ Gaussian fit by $\pm 0.2$ GeV as in \cite{PHENIX:2018trr}. We see that the best description of both the 200 GeV and the 510 GeV data is obtained with the CGC w Sud computation. In Fig.~\ref{fig:ktbroad} we also plot Sud results for the Gaussian widths and find that they are below the PHENIX data. The CGC w/o Sud widths are not shown - due to the double peak structure the behavior is clearly not Gaussian-like for small $p_{\rm out}$. But even if we choose to ignore this issue, based on the fact that the double peak is rather narrow for this particular kinematics, it is visible already by the naked eye from Fig.~\ref{fig:poutdist} that the distribution are too narrow in comparison to the data.

\begin{figure}
  \begin{center}
  \includegraphics[scale = 0.6]{gwidths_pred.pdf}
  \end{center}
  \caption{The difference between $pA$ and $pp$ Gaussian widths squared of the $p_{\rm out}$ distributions as a function of $x_E$ at $\sqrt{s}=200$ GeV and $\sqrt{s}=5.02$ TeV collision energies.}
  \label{fig:ktbroad2}
\end{figure}

In Fig.~\ref{fig:ktbroad2}, as a measure of the nuclear effect, we show our predictions for the difference in the Gaussian widths squared computed in mid-rapidity $pA$ and in $pp$ at RHIC (left) and at the LHC (right) kinematics. For convenience we denote this quantity as $\langle p_{\rm out}^2  \rangle_{pA} - \langle p_{\rm out}^2 \rangle_{pp}$, though the meaning of the ``averaging" procedure $\langle \,\, \rangle$ is in the sense of fitting the small $p_{\rm out}$ region with a Gaussian - same as we used for Fig.~\ref{fig:ktbroad}. Our choice of kinematics matches the one used in the preliminary RHIC $p$Pb vs. $pp$ results in \cite{Osborn:2017ndr,Osborn:2018bwn,Aidala:2019sok} with the hard scale $5 \, {\rm GeV}<k_{\gamma\perp} < 9 \, {\rm GeV}$ and we plot our results as a function of $x_E$. We are tempted to compare the $200$ GeV results from Fig.~\ref{fig:ktbroad2} with the preliminary result in Refs.~\cite{Osborn:2017ndr,Osborn:2018bwn,Aidala:2019sok} that shows up to about $0.1$ GeV$^2$ broader widths in $pA$ that in $pp$, for $x_E < 0.4$, albeit for $\pi^0 h^\pm$ production. In our $\gamma h^\pm$ computation we find $\lesssim 0.15$ GeV$^2$ for $x_E < 0.4$.  Increasing the energy to $5.02$ TeV we find that the difference in the $pA$ vs. $pp$ Gaussian widths grows, becoming more pronounced at large $x_E$.

\section{Conclusions}
\label{sec:conc}

In this paper we have numerically computed the isolated photon-hadron production cross section based on the leading order CGC formula with the Sudakov resummation explicitly taken into account for the first time. We have demonstrated that both the CGC and the Sudakov effects are important to obtain a reasonable description of the data at RHIC and the LHC. We have provided predictions for the nuclear suppression around the away side peak $\Delta \phi = \pi$ and the nuclear broadening of the intrinsic transverse momentum distributions at RHIC and at the LHC. While the PHENIX collaboration published only $pp$ data, the ALICE collaboration has results also for $pp$ and $p$Pb. Unfortunately, there is no clear evidence of a nuclear effect from the data alone. This might be due to asymmetric $k_{\gamma\perp} \times P_{h\perp}$ binning by ALICE and we argue that in more symmetric configurations the nuclear effect would be more apparent.
In addition to $\gamma h^\pm $ production the PHENIX experiment measured also $\pi^0 h^\pm$ production \cite{PHENIX:2016zxb,PHENIX:2018trr}. The data seems to indicate a suppression in the $\gamma h^\pm$ vs. $\pi^0 h^\pm$ production in the bins that are close to the away side peak. It would be interesting to make a detailed side-by-side comparison of $\gamma h^\pm$ vs. $\pi^0 h^\pm$ production in CGC.

As a future work we plan to take into account next-to-leading order corrections which bring $2 \to 3$ partonic processes into play. Firstly, already in the collinear framework, the presence of an additional (unobserved) parton present in the final state naturally disrupts the $\gamma h$ back-to-back kinematics. As the Sudakov effect is associated with soft gluon branching it is most important in the region close to the away side peak with the momentum imbalance $k_\perp = |\boldsymbol{q}_\perp + \kgp|$ such that $k_\perp \ll Q$. By contrast, the $2 \to 3$ processes are genuine hard branchings, that are able to support large momentum imbalances $k_\perp \sim Q$. Therefore, next-to-leading order corrections and Sudakov effects are important to get a more complete phase-space picture of $\gamma h$ correlations. This has recently been applied in describing hard-$p_\perp$ $\gamma$-jet data in $pp$, see e.~g.~\cite{Jezo:2016ypn,Klasen:2017dsy} and also \cite{Chen:2018fqu}. We also mention here recent works on transverse momentum resummation in $\gamma$-jet production that also takes into account a preferred direction set by the final state jet \cite{Buffing:2018ggv,Hatta:2021jcd}.

In the small-$x$ kinematics region with $k_\perp \sim Q_S$ we are interested, a complete next-to-leading order treatment would include considering the $g g \to q\bar{q}\gamma$ \cite{Benic:2016uku,Benic:2016yqt} and $qg \to qg \gamma$ channels \cite{Altinoluk:2018uax,Altinoluk:2018byz} (see also \cite{Roy:2018jxq,Roy:2019hwr} for related higher order computations in $eA$ collisions). With the current photon detectors in the mid-rapidity region for both RHIC and LHC, as a first step, the inclusion of the $g g \to q\bar{q}\gamma$ channel might be enough. Considering planned forward upgrades \cite{ALICE:2020mso,Berti:2021azk}, where the isolated photon signal would be more favourably extracted from the $\pi^0$ background, taking into account also the $qg \to qg \gamma$ channel becomes important.

\acknowledgments

We thank Abhiram Kaushik for discussions. S.~B. thanks Yoshitaka Hatta, Joseph Osborn, Sebastian Sapeta and Shu-yi Wei for very useful correspondences. S.~B. and A.~P. are supported by the Croatian Science Foundation (HRZZ) no. 5332 (UIP-2019-04).  This project was supported by  the Deutsche Forschungsgemeinschaft (DFG, German Research Foundation) – Project number 315477589 – TRR 211.

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