193 research outputs found

    HYSTEROSALPINGOGRAPHY: TECHNIQUE AND APPLICATIONS (VIEW)

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    Hysterosalpingography (HSG) is the radiographic evaluation of the uterine cavity and fallopian tubes after the administration of a radio-opaque medium through the cervical canal. The first HSG was performed in 1910 and was considered to be the first special radio¬logic procedure. A properly performed HSG can de¬tect the contour of the uterine cavity and the width of the cervical canal. Further contrast medium injection will outline the cornua isthmic and ampullary portions of the tubes, and will show the degree of spillage. If a properly performed HSG shows no uterine cavity abnormality, it is very unlikely that other modalities would do so. Although this procedure is considered diagnostic, there may also be a possible therapeutic benefit from the flushing effect. Indications and Contraindications HSG is used predominantly in the evaluation of in-fertility. Despite the arrival of newer imaging modalities, HSG still remains the best procedure to image the fallopi¬an tubes. Although evaluating feminine infertility, with or without the presence of repeated miscarriages, is the main indication for this method, it can also be used in other cas-es, such as pain in the pelvis tract, congenital or anatomic abnormalities, anomalies of the menstrual cycle, and ab-normal menses. Also, it is sometimes used as a preoper-ative control for women who are about to have uterine or tubal surgery. Soares and coworkers showed that HSG had a sensitivity of 58% and a positive-predictive value of 28.6% for polypoid lesions, and a sensitivity of 0% for endometrial hyperplasia. The same study showed HSG to have a sensitivity of 44.4% for uterine malformations, and a sensitivity of 75% for the detection of intrauterine adhesions. The main contraindication of the examination is possible pregnancy. This contraindication can be avoid¬ed by performing the examination before the ovulation phase, between the 7th to 10th day of the menstrual cycle. Because of the scattering risk, the examination should be avoided when there is active intrapelvic inflammation. Another contraindication is vaginal or uterine bleeding because of the risk of unrestrained bleeding, which could lead to transfusion or surgical recovery procedures. Fi¬nally, the examination should not be performed in cases of severe cardiac or renal deficiency, or in cases of recent uterine or tubal surgery. Technique Patient Preparation The procedure is performed in the first half of the menstrual cycle following cessation of bleeding. The endometrium is thin during this proliferative phase, which facilitates better image interpretation and should also ensure that there is no pregnancy. The patient is asked to refrain from unprotected sexual intercourse from the date of her period until after the investigation to be certain there is no risk of pregnancy. Examination in the second half of the cycle is avoided because the thickened secretory-phase endometrium increases the risk of venous intravasation and may cause a false-pos¬itive diagnosis of cornual occlusion. Antibiotics might be required 1 day before and for a few days after the examination if previous inflamma¬tions are present in the patient’s clinical history. Antibiotics are required after the examination when the maneuvers are fairly sanguineous or if the fallopian tubes present a certain degree of dilation. The suggest¬ed antibiotic regimen is metronidazole 1 g rectally at the time of the procedure, plus doxycycline 100 mg twice daily for 7 days.Steroid (prednisolone) premed¬ication is prescribed in asthmatics when intravenous contrast is used; there-fore, it is reasonable to do the same for HSG because intravasation is also possible from this procedure. Catheterization Technique For the catheterization technique, the patient is placed on the fluoroscopic machine in a gynecologic examination position. After cleaning the external gen¬ital area with antiseptic solution, the vagina is dilated by a gynecologic dilator. The cervix is localized and cleansed with iodine solution. Afterward, the uterine cervix is straightened by one (at the 12 o’clock posi¬tion) or two (at the 9 and 3 o’clock positions) surgi¬cal forceps exercising a degree of pulling. Next, the outside uterine cervix ostium is catheterized. The catheterization can be performed in two ways. In the authors’ country, a salpinographer with a bell-shaped end (diameter depends on the case) is pushed through the vagina and fits in the external uterine cervix osti¬um. In the second technique, the salpingographer has a plastic cup-shaped end that is fitted to the external uterine cervix ostium, creating a void phenomenon. In both techniques, there is a syringe with iodinated hydrosoluble contrast medium at the other end of the salpingographer. The vagina dilator is taken off after catheterization of the external uteri cervix ostium and before administration of the contrast medium. Contrast Media In the past, oil-soluble contrast media were mainly used. Today, we use all available iodinated hydrosol¬uble contrast media. According to international liter¬ature, the use of oil-soluble contrast media increases the pregnancy rate and contributes to a decrease in conception time after the salpingography is performed. However, Spring and coworkers found that there is no evidence that the choice of the contrast material affects the rate of term pregnancy. Moreover, they reported that oil-soluble contrast media may promote granulo¬matous inflammation in the presence of obstructed or inflamed fallopian tubes. Radiological Views One conventional radiograph of the pelvis (on a 24¬30 cm radiologic film) is necessary before the contrast medium is administrated into the uterine cavity so that possible intrapyelic masses or calcifications will not complicate interpretation of the images. A metallic marker is placed over one side of the pelvis to indicate the right or left side of the patient. Next, the examina¬tion is performed under fluoroscopic control so that ra¬diographs can be taken during the filling of the uterine cavity (usually 2-3 cm of contrast medium is sufficient) and again during the filling of the fallopian tubes. Final¬ly, after the removal of the salpingographer, we radio¬graphically check the presence of contrast medium in the peritoneal cavity. The total amount of injected con¬trast medium should not exceed 10 mL. Additional spot radiographs are obtained to document any abnormality that is seen. Before the first radiograph, we also fluoro- scopically check the reflux of the contrast medium. Complications The two most common complications of HSG are pain and infection. These and other complications and side effects are summarized below. • Uterine contractions and discomfort due to the introduction of contrast medium into the uterine cavi¬ty: The most common type of pain referenced is subab¬dominal colic caused by dilation of the uterine cavity. A more diffuse pain, caused by irritation of the peri¬toneum due to the contrast medium, has also been re¬ported. Pain can be minimized by slowly injecting the contrast medium and using isosmolar contrast agents. • Postprocedural infection: Spreading and gener-alization of intrapyelic inflammation may happen in cases of chronic inflammation and hydrosalpinges, or after severe uterine injury caused by the examination maneuver. • Vasovagal reaction: A possible reaction to ma-nipulation of the cervix or inflation of a conclusion balloon in the cervical canal. • Traumatic elevation of endometrium by the in¬serted cannula: A complication which does not cause significant consequences. • Uterine perforation and tubal rupture: These complications are very rare. • Venous or lymphatic intravasation of contrast me-dia: With a water-based contrast medium there is no ad-verse effect on the patient, but it can make interpretation of the image difficult. It occurs more commonly in the presence of fibroids or tubal obstruction. Extravasation of the contrast medium could occur if the contrast me¬dium is administered too quickly, if the endometrium is injured during the catheterization, or if the examination is performed during menstruation. Extravasation is also possible when common or special inflammations of the endometrium are present due to the intercourse rate be-tween the uterine vein and the ovarian veins. • Allergic reaction to contrast media: Such a reac¬tion is very uncommon with the use of the low-osmolar nonionic contrast agents currently available. • Radiation exposure to the ovaries: Exposure is minimal and can be reduced if the proper technique is utilized. Normal Findings On face radiographs, the uterine cavity has a nor¬mal trigonal shape and the apex of the triangle corre¬sponds to the isthmus, which is nearly 3.7 cm wide. The apex is pointed downwards and connected to the internal ostium of the cervix uteri, which is 2.5 cm in total length. The base of triangular uterine cavity is the fundus, which can be concave, flattened, or slightly convex. On both sides of its base, in the area of the lateral horns, the two fallopian tubes are drowned. The fallopian tubes are separated into three segments: isth¬mus (attached to the uterus, not imaged in several cas¬es), ampullary (in the middle, the longest and widest segment), and bell-shaped (to the distal end). There are two ostiums: the internal or uterine, and the external or abdominal. From the abdominal ostium, the con¬trast medium disperses and diffuses into the peritone¬al cavity. Remaining contrast medium in the furrows of the peritoneum can be observed up to 3 hours after administration. Very often, the contrast medium in the rectouterine pouch of the peritoneum (Douglas’ space) can demonstrate the profile of the coordinate ovary. Congenital Uterus Anomalies Congenital uterus anomalies are caused by incom¬plete junction of the paramesonephric ducts (Muller ducts), or Extravasations of the contrast medium. The true incidence and prevalence of mullerian duct anomalies are difficult to assess. Examination of different patient populations, nonstandardized clas¬sification systems, and differences in diagnostic data acquisition has resulted in widely disparate estimates, with a reported prevalence that ranges from 0.16 to 10%. As a result of selection bias, a prevalence of 8 to 10% has been reported in women being evaluated with HSG because of recurrent pregnancy loss. The overall data suggest that the prevalence both in women with normal fertility and in women with infertility is approximately 1%, and the prevalence in women with repeated pregnancy loss is approximately 3%. While the majority of women with mullerian duct anomalies have little problem conceiving, they have higher associated rates of spontaneous abortion, pre¬mature delivery, and abnormal fetal position and dys¬tocia at delivery. Most studies report an approximate frequency of 25% for associated reproductive prob¬lems, compared with 10% in the general population. Primary infertility in these women usually has an ex¬tra uterine cause and is not generally attributable to mullerian duct anomalies alone. Additionally, cervical incompetence has been reported to be associated with these anomalies. According to the American Society of Reproduc¬tive Medicine, there are seven different classes of mul¬lerian duct anomalies: Class I: Segmental agenesis or variable degrees of uterovaginal hypoplasia. The anomaly can be detected, because of the amenorrhea, before HSG is performed. Class II: Unicornuate uteri that represent partial or complete unilateral hypoplasia. In rare cases of degen-eration of the mesonephric duct, the uterine cavity ap¬pears monocular when imaged, placed right or left of the middle line. The unicornuate uterus contacts only the coordinate fallopian tube. Class III: Didelphys uterus. This is a rare abnor¬mality that results from complete nonfusion of the mullerian ducts, and includes the duplication of the uterine cavity, cervix neck, and vagina. Rarely, this uterus has a single vagina. Class IV: Bicornuate uterus that demonstrates incomplete fusion of the superior segments of the uterovaginal canal. The uterine cavity is divided in two; each half has a narrow-length shape and stands apart from the other. Class V: Septate uteri that represent partial or com¬plete nonresorption of the uterovaginal septum. Class VI: Arcuate uterus resulting from nearly complete resorption of the septum. Along with the pre¬vious anomaly, these are the most common congenital anomalies (50%) in cases detecting female infertility. Class VII: Anomalies that comprise sequelae of in utero diethyloestradiol exposure. Another congenital anomaly, caused by inadequate hormonic stimulation as a fetus, is small uterine cavi¬ty size with normal vaginal length. This is a common finding in cases of female infertility. Abnormal Findings Fibromyomas While fibromas are diagnosed by suprapubic ultra-sound, submucosa fibromyomas are imaged as smooth filling defects in the uterine cavity. Differential diagno¬sis must be made from endometrial polyps or possible pregnancy. Small intramural fibromyomas do not distort the endometrial cavity and are not visualized on HSG. Subserous fibromyomas can provoke smooth filling de-fects or smooth repression of the fallopian tubes only if they are located in the lateral walls of the uterus. Endometrial Polyps Endometrial polyps are focal overgrowths of the endometrium. They usually manifest as well-defined filling defects and are best seen during the early filling stage. Small polyps may be obscured when contrast material completely fills the uterine cavity and may be indistinguishable from a small submucosal myoma. Sonohysterography has become the preferred method of imaging endometrial polyps. Internal Endometriosis (Adenomyosis) Adenomyosis is caused by the presence of ectopic islets of active endometrium in the muscularis wall of the uterus. It is usually imaged as a pointed projection of 2 to 3 mm length, perpendicular to the uterine wall after contrast medium administration. Rarely, this is imaged as a sack-shaped projection filled by contrast medium, 4 mm to 1 cm in length. Differential diag¬nosis should include the hyperplasia of the endome¬trium and the entrance of the contrast medium in the myometrium or in the nutrient arteriole of submucosa fibromyomas. Uterine Cancer Uterine cancer manifests as an irregular filling de¬fect, but is rarely diagnosed by the HSG method. Intrauterine Adhesions Intrauterine adhesions are most commonly caused by endometrial trauma of curettage. They are also seen in patients with chronic endometriosis due to tubercu¬losis. Genital tuberculosis primary affects the fallopian tubes, and 50% of patients with tubal disease also have a uterine abnormality. Intrauterine adhesions manifest as irregular filling defects, most commonly as linear filling defects arising from one of the uterine walls. Hydrosalpinx HSG is the best method for visualizing and eval¬uating the fallopian tubes. Hydrosalpinx is a common finding that results from a previous inflammation of the fallopian tubes (salpingitis). This is usually the se¬quelae of distal tubal occlusion, leading to dilation of the proximal segment. The radiologic image shows a dilated lumen in one or more spots, and the contrast medium will not make its way to the peritoneal cavity Tuberculated Salpingitis This entity usually causes distant fallopian tube end obliteration. In extensive infections, multiple con¬strictions along the course of fallopian tube can form, resulting in areas of dilation and stenosis. Abnormal uterine and vaginal profiles are observed in cases of widespread infection. Salpingitis Isthmica Nodosa Salpingitis isthmica nodosa is a disease of un¬known etiology, characterized by multiple small out- pouchings or diverticula affecting one or both fallopian tubes. It is presumably caused by pelvic inflammatory disease or endometriosis and is associated with ectopic pregnancy and infertility. Nondrawing of the Fallopian Tubes This is the most common finding during the exam-ination and is usually caused by poor technique, spasm, or obliteration of the fallopian tube. Poor technique in¬cludes imperfect straightening of the external cervical ostium or an inadequate amount of contrast medium in the uterine cavity. The cornual portion of the fallopian tube is encased by the smooth muscle of the uterus and, if there is a spasm of the muscle during HSG, one or both tubes may not fill. Using radiography, tubal spasm cannot be distinguished from tubal occlusion. This could be avoided by progressive administration of the contrast medium or, when the spasm occurs, administration of a spasmolytic agent to relieve spasm, helping differentiate cornual spasm from true occlusion. Obliteration is usu¬ally caused by previous inflammation or uterine surgery and manifests as nonopacification or abrupt cutoff of the fallopian tube with no free intraperitoneal spillage. External Adhesions External adhesions occur secondary to previous inflammation or surgery, similar to the causes of tubal occlusion. Peritubal adhesions prevent contrast materi¬al from flowing freely around the bowel loops as seen in normal cases, and most commonly manifest as loc- ulation of the contrast material around the ampullary portion of the tube. Conclusion. HSG remains the front-line imaging modality in the investigation of infertility. It is an ac¬curate means of accessing the uterine cavity and tubal patency, but has a low sensitivity for the diagnosis of pelvic adhe¬sions, which is why it cannot replace laparoscopy. It requires knowledge of the female anatomy as well as skillful technique in order to avoid pitfalls and misin¬terpretations.Кафедра акушерства та гінекологі

    A physical and regulatory map of host-influenza interactions reveals pathways in H1N1 infection

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    available in PMC 2010 June 28.During the course of a viral infection, viral proteins interact with an array of host proteins and pathways. Here, we present a systematic strategy to elucidate the dynamic interactions between H1N1 influenza and its human host. A combination of yeast two-hybrid analysis and genome-wide expression profiling implicated hundreds of human factors in mediating viral-host interactions. These factors were then examined functionally through depletion analyses in primary lung cells. The resulting data point to potential roles for some unanticipated host and viral proteins in viral infection and the host response, including a network of RNA-binding proteins, components of WNT signaling, and viral polymerase subunits. This multilayered approach provides a comprehensive and unbiased physical and regulatory model of influenza-host interactions and demonstrates a general strategy for uncovering complex host-pathogen relationships.National Institutes of Health (U.S.) (grant U01 AI074575)National Institutes of Health (U.S.) (grant U54 AI057159)National Institutes of Health (U.S.) (NIH New Innovator Award)Ford Foundation (Predoctoral Fellowship)Ellison Medical FoundationNational Institutes of Health (U.S.) (NIH grant R01 HG001715)National Institutes of Health (U.S.) (grant P50 HG004233)National Institutes of Health (U.S.) (PIONEER award)Howard Hughes Medical InstituteBurroughs Wellcome Fund (Career Award at the Scientific Interface)Alfred P. Sloan Foundatio

    Search for direct production of charginos and neutralinos in events with three leptons and missing transverse momentum in √s = 7 TeV pp collisions with the ATLAS detector

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    A search for the direct production of charginos and neutralinos in final states with three electrons or muons and missing transverse momentum is presented. The analysis is based on 4.7 fb−1 of proton–proton collision data delivered by the Large Hadron Collider and recorded with the ATLAS detector. Observations are consistent with Standard Model expectations in three signal regions that are either depleted or enriched in Z-boson decays. Upper limits at 95% confidence level are set in R-parity conserving phenomenological minimal supersymmetric models and in simplified models, significantly extending previous results

    Jet size dependence of single jet suppression in lead-lead collisions at sqrt(s(NN)) = 2.76 TeV with the ATLAS detector at the LHC

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    Measurements of inclusive jet suppression in heavy ion collisions at the LHC provide direct sensitivity to the physics of jet quenching. In a sample of lead-lead collisions at sqrt(s) = 2.76 TeV corresponding to an integrated luminosity of approximately 7 inverse microbarns, ATLAS has measured jets with a calorimeter over the pseudorapidity interval |eta| < 2.1 and over the transverse momentum range 38 < pT < 210 GeV. Jets were reconstructed using the anti-kt algorithm with values for the distance parameter that determines the nominal jet radius of R = 0.2, 0.3, 0.4 and 0.5. The centrality dependence of the jet yield is characterized by the jet "central-to-peripheral ratio," Rcp. Jet production is found to be suppressed by approximately a factor of two in the 10% most central collisions relative to peripheral collisions. Rcp varies smoothly with centrality as characterized by the number of participating nucleons. The observed suppression is only weakly dependent on jet radius and transverse momentum. These results provide the first direct measurement of inclusive jet suppression in heavy ion collisions and complement previous measurements of dijet transverse energy imbalance at the LHC.Comment: 15 pages plus author list (30 pages total), 8 figures, 2 tables, submitted to Physics Letters B. All figures including auxiliary figures are available at http://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HION-2011-02

    Search for strong gravity in multijet final states produced in pp collisions at √s=13 TeV using the ATLAS detector at the LHC

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    A search is conducted for new physics in multijet final states using 3.6 inverse femtobarns of data from proton-proton collisions at √s = 13TeV taken at the CERN Large Hadron Collider with the ATLAS detector. Events are selected containing at least three jets with scalar sum of jet transverse momenta (HT) greater than 1TeV. No excess is seen at large HT and limits are presented on new physics: models which produce final states containing at least three jets and having cross sections larger than 1.6 fb with HT > 5.8 TeV are excluded. Limits are also given in terms of new physics models of strong gravity that hypothesize additional space-time dimensions

    Operation and performance of the ATLAS semiconductor tracker

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    The semiconductor tracker is a silicon microstrip detector forming part of the inner tracking system of the ATLAS experiment at the LHC. The operation and performance of the semiconductor tracker during the first years of LHC running are described. More than 99% of the detector modules were operational during this period, with an average intrinsic hit efficiency of (99.74±0.04)%. The evolution of the noise occupancy is discussed, and measurements of the Lorentz angle, δ-ray production and energy loss presented. The alignment of the detector is found to be stable at the few-micron level over long periods of time. Radiation damage measurements, which include the evolution of detector leakage currents, are found to be consistent with predictions and are used in the verification of radiation background simulations

    Measurement of the correlation between flow harmonics of different order in lead-lead collisions at √sNN = 2.76 TeV with the ATLAS detector

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    Correlations between the elliptic or triangular flow coefficients vm (m=2 or 3) and other flow harmonics vn (n=2 to 5) are measured using √sNN=2.76 TeV Pb+Pb collision data collected in 2010 by the ATLAS experiment at the LHC, corresponding to an integrated luminosity of 7 μb−1. The vm−vn correlations are measured in midrapidity as a function of centrality, and, for events within the same centrality interval, as a function of event ellipticity or triangularity defined in a forward rapidity region. For events within the same centrality interval, v3 is found to be anticorrelated with v2 and this anticorrelation is consistent with similar anticorrelations between the corresponding eccentricities, ε2 and ε3. However, it is observed that v4 increases strongly with v2, and v5 increases strongly with both v2 and v3. The trend and strength of the vm−vn correlations for n=4 and 5 are found to disagree with εm−εn correlations predicted by initial-geometry models. Instead, these correlations are found to be consistent with the combined effects of a linear contribution to vn and a nonlinear term that is a function of v22 or of v2v3, as predicted by hydrodynamic models. A simple two-component fit is used to separate these two contributions. The extracted linear and nonlinear contributions to v4 and v5 are found to be consistent with previously measured event-plane correlations

    Search for H→γγ produced in association with top quarks and constraints on the Yukawa coupling between the top quark and the Higgs boson using data taken at 7 TeV and 8 TeV with the ATLAS detector

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    A search is performed for Higgs bosons produced in association with top quarks using the diphoton decay mode of the Higgs boson. Selection requirements are optimized separately for leptonic and fully hadronic final states from the top quark decays. The dataset used corresponds to an integrated luminosity of 4.5 fb−14.5 fb−1 of proton–proton collisions at a center-of-mass energy of 7 TeV and 20.3 fb−1 at 8 TeV recorded by the ATLAS detector at the CERN Large Hadron Collider. No significant excess over the background prediction is observed and upper limits are set on the tt¯H production cross section. The observed exclusion upper limit at 95% confidence level is 6.7 times the predicted Standard Model cross section value. In addition, limits are set on the strength of the Yukawa coupling between the top quark and the Higgs boson, taking into account the dependence of the tt¯H and tH cross sections as well as the H→γγ branching fraction on the Yukawa coupling. Lower and upper limits at 95% confidence level are set at −1.3 and +8.0 times the Yukawa coupling strength in the Standard Model

    The performance of the jet trigger for the ATLAS detector during 2011 data taking

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    The performance of the jet trigger for the ATLAS detector at the LHC during the 2011 data taking period is described. During 2011 the LHC provided proton–proton collisions with a centre-of-mass energy of 7 TeV and heavy ion collisions with a 2.76 TeV per nucleon–nucleon collision energy. The ATLAS trigger is a three level system designed to reduce the rate of events from the 40 MHz nominal maximum bunch crossing rate to the approximate 400 Hz which can be written to offline storage. The ATLAS jet trigger is the primary means for the online selection of events containing jets. Events are accepted by the trigger if they contain one or more jets above some transverse energy threshold. During 2011 data taking the jet trigger was fully efficient for jets with transverse energy above 25 GeV for triggers seeded randomly at Level 1. For triggers which require a jet to be identified at each of the three trigger levels, full efficiency is reached for offline jets with transverse energy above 60 GeV. Jets reconstructed in the final trigger level and corresponding to offline jets with transverse energy greater than 60 GeV, are reconstructed with a resolution in transverse energy with respect to offline jets, of better than 4 % in the central region and better than 2.5 % in the forward direction

    Measurement of event-shape observables in Z→ℓ+ℓ− events in pp collisions at √ s=7 TeV with the ATLAS detector at the LHC

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    Event-shape observables measured using charged particles in inclusive ZZ-boson events are presented, using the electron and muon decay modes of the ZZ bosons. The measurements are based on an integrated luminosity of 1.1fb11.1 {\rm fb}^{-1} of proton--proton collisions recorded by the ATLAS detector at the LHC at a centre-of-mass energy s=7\sqrt{s}=7 TeV. Charged-particle distributions, excluding the lepton--antilepton pair from the ZZ-boson decay, are measured in different ranges of transverse momentum of the ZZ boson. Distributions include multiplicity, scalar sum of transverse momenta, beam thrust, transverse thrust, spherocity, and F\mathcal{F}-parameter, which are in particular sensitive to properties of the underlying event at small values of the ZZ-boson transverse momentum. The Sherpa event generator shows larger deviations from the measured observables than Pythia8 and Herwig7. Typically, all three Monte Carlo generators provide predictions that are in better agreement with the data at high ZZ-boson transverse momenta than at low ZZ-boson transverse momenta and for the observables that are less sensitive to the number of charged particles in the event.Comment: 36 pages plus author list + cover page (54 pages total), 14 figures, 4 tables, submitted to EPJC, All figures including auxiliary figures are available at http://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/STDM-2014-0
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