1,536 research outputs found
Modeling missing transverse energy in V+jets at CERN LHC
I discuss a method to model the instrumental response of the CMS and ATLAS
detectors at high transverse missing energies to dominant standard model V+jets
backgrounds, where V is a Z, gamma or W, using multi-jet QCD events. The method
is developed for new physics searches in early data at the Large Hadron
Collider (LHC) with minimal recourse to simulation.Comment: Replaced with the published versio
INFLUENCE OF MEDICO-SOCIAL RISK FACTORS ON PSYCHOEMOTICAL STATE AND SELF-ESTEEM OF FEMALE PATIENTS OF REPRODUCTIVE AGE WITH TUBERCOLOSIS OF THE RESPIRATORY SYSTEM
Aim - to study the influence of medical and social risk factors on the psychoemotional state and selfesteem of female patients of reproductive age with tuberculosis of the respiratory system. Material and methods. The main group consisted of 93 women aged 18-44 with tuberculosis of the respiratory system who received treatment in one of the anti-tuberculosis institutions of the Nizhny Novgorod region in 2013. The comparison group consisted of 82 almost healthy women of the corresponding age. To assess the psychoemotional state, we carried out a survey using the SAM test method (state of health, activity, mood); to evaluate personality traits - the test Β«Self-assessment of the personalityΒ» by O.I. Motkov. The questionnaire included additional questions of medical and social nature. Results. It was proven that the presence of unfavorable medical and social risk factors in this category of patients causes a decrease in self-evaluation of the positive aspects of the personality, and has a negative impact on the psychoemotional state of patients, causing poor health (lowest evaluated), low activity, bad mood. In the course of long-term treatment, women feel tired and exhausted. Among the medical and social risk factors that have adverse impact on the psychoemotional state and self-esteem of women, the following factors should be highlighted: low level of education, poor financial situation, lack of awareness about prophylaxis of tuberculosis, intense interpersonal relationships in the family, frequent exposure to stress and rueful feelings, irregularity of the prophylactic chest X-ray examinations, violation of the work-rest regime, dietary regimen and quality of nutrition, the history of tubercular contact and incarceration. Conclusion. The results of the research demonstrate the need for developing and implementation of measures of providing psychological assistance to the female patients of reproductive age with active tuberculosis of the respiratory system, as well as new approaches to the prevention of this disease, based on established psychological risk factors for the emergence of tuberculous process and its recurrence
Study of LHC Searches for a Lepton and Many Jets
Searches for new physics in high-multiplicity events with little or no
missing energy are an important component of the LHC program, complementary to
analyses that rely on missing energy. We consider the potential reach of
searches for events with a lepton and six or more jets, and show they can
provide increased sensitivity to many supersymmetric and exotic models that
would not be detected through standard missing-energy analyses. Among these are
supersymmetric models with gauge mediation, R-parity violation, and light
hidden sectors. Moreover, ATLAS and CMS measurements suggest the primary
background in this channel is from t-tbar, rather than W+jets or QCD, which
reduces the complexity of background modeling necessary for such a search. We
also comment on related searches where the lepton is replaced with another
visible object, such as a Z boson.Comment: 23 pages, 12 figures, 1 tabl
ΠΠ΅Ρ Π°Π½ΠΈΠ·ΠΌΡ ΡΠ°Π·Π²ΠΈΡΠΈΡ Π»Π΅ΠΊΠ°ΡΡΡΠ²Π΅Π½Π½ΠΎΠΉ ΡΡΡΠΎΠΉΡΠΈΠ²ΠΎΡΡΠΈ Mycobacterium tuberculosis: Π΅ΡΡΡ Π»ΠΈ ΡΠ°Π½Ρ ΠΏΠΎΠ±Π΅Π΄ΠΈΡΡ?
The scientific review provides current information on the current epidemiological status of tuberculosis in our country and the world, genetic adaptability and the evolution of Mycobacterium tuberculosis. The well-known and recently discovered molecular targets of aggression of this microorganism are described, and possible methods of circumventing the resistance of the Office to existing and developed drugs are presented. Objective: to create a scientific analytical review, which allows you to form an idea of the basic principles of development of the mechanisms of drug resistance of M. tuberculosis, as well as ways to overcome them with the possibility of further development of the chosen direction with the involvement of reputable scientific groups and practical implementation. Methods. scientific analysis of international reports, highly indexed scientific articles and clinical protocols. Results. Ihanks to the conducted analytical work, critical biological markers of M. tuberculosis immunity to anti-tuberculosis therapy were identified, which protect it from pharmacological intervention by the person and do not adequately sanitize the centers of inflammation in the patient's body. Methods have been proposed for disintegrating the mechanisms of drug resistance, which will bring the algorithms for treating tuberculosis infection to a new level. Conclusion. The analyzed information will contribute to deepening and expanding the knowledge of specialists involved in the fight against tuberculosis about the importance of implementing a personalized approach in the provision of medical care to TB patients, taking into account the studied molecular indicators of resistance to standardized and developed drugs.Π Π½Π°ΡΡΠ½ΠΎΠΌ Π°Π½Π°Π»ΠΈΡΠΈΡΠ΅ΡΠΊΠΎΠΌ ΠΎΠ±Π·ΠΎΡΠ΅ ΠΏΡΠ΅Π΄ΡΡΠ°Π²Π»Π΅Π½Π° Π°ΠΊΡΡΠ°Π»ΡΠ½Π°Ρ ΠΈΠ½ΡΠΎΡΠΌΠ°ΡΠΈΡ ΠΎ ΡΠΎΠ²ΡΠ΅ΠΌΠ΅Π½Π½ΠΎΠΌ ΡΠΏΠΈΠ΄Π΅ΠΌΠΈΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΎΠΌ ΡΡΠ°ΡΡΡΠ΅ ΠΏΠΎ ΡΡΠ±Π΅ΡΠΊΡΠ»Π΅Π·Ρ Π² Π½Π°ΡΠ΅ΠΉ ΡΡΡΠ°Π½Π΅ ΠΈ ΠΌΠΈΡΠ΅, Π³Π΅Π½Π΅ΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΏΡΠΈΡΠΏΠΎΡΠ°Π±Π»ΠΈΠ²Π°Π΅ΠΌΠΎΡΡΠΈ ΠΈ ΡΠ²ΠΎΠ»ΡΡΠΈΠΎΠ½ΠΈΡΠΎΠ²Π°Π½ΠΈΠΈ Mycobacterium tuberculosis. ΠΠΏΠΈΡΠ°Π½Ρ ΠΈΠ·Π²Π΅ΡΡΠ½ΡΠ΅ ΠΈ Π½Π΅Π΄Π°Π²Π½ΠΎ ΠΎΡΠΊΡΡΡΡΠ΅ ΠΌΠΎΠ»Π΅ΠΊΡΠ»ΡΡΠ½ΡΠ΅ ΠΌΠΈΡΠ΅Π½ΠΈ Π°Π³ΡΠ΅ΡΡΠΈΠΈ Π΄Π°Π½Π½ΠΎΠ³ΠΎ ΠΌΠΈΠΊΡΠΎΠΎΡΠ³Π°Π½ΠΈΠ·ΠΌΠ°, ΠΏΡΠ΅Π΄ΡΡΠ°Π²Π»Π΅Π½Ρ Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΡΠ΅ ΠΌΠ΅ΡΠΎΠ΄ΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΠΏΡΠΈΠ΅ΠΌΡ ΠΎΠ±Ρ
ΠΎΠ΄Π° Π½Π΅Π²ΠΎΡΠΏΡΠΈΠΈΠΌΡΠΈΠ²ΠΎΡΡΠΈ ΠΌΠΈΠΊΠΎΠ±Π°ΠΊΡΠ΅ΡΠΈΠΈ ΡΡΠ±Π΅ΡΠΊΡΠ»Π΅Π·Π° (ΠΠΠ’) ΠΊ ΡΡΡΠ΅ΡΡΠ²ΡΡΡΠΈΠΌ ΠΈ ΡΠ°Π·ΡΠ°Π±Π°ΡΡΠ²Π°Π΅ΠΌΡΠΌ ΠΏΡΠ΅ΠΏΠ°ΡΠ°ΡΠ°ΠΌ. Π¦Π΅Π»ΡΡ ΠΎΠ±Π·ΠΎΡΠ° ΡΠ²ΠΈΠ»ΠΎΡΡ ΡΠΎΡΠΌΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅ ΠΏΡΠ΅Π΄ΡΡΠ°Π²Π»Π΅Π½ΠΈΡ ΠΎ ΠΏΡΠΈΠ½ΡΠΈΠΏΠ°Ρ
ΡΠ°Π·Π²ΠΈΡΠΈΡ ΠΌΠ΅Ρ
Π°Π½ΠΈΠ·ΠΌΠΎΠ² Π»Π΅ΠΊΠ°ΡΡΡΠ²Π΅Π½Π½ΠΎΠΉ ΡΠ΅Π·ΠΈΡΡΠ΅Π½ΡΠ½ΠΎΡΡΠΈ ΠΠΠ’, Π° ΡΠ°ΠΊΠΆΠ΅ ΡΠΏΠΎΡΠΎΠ±Π°Ρ
, ΠΏΠΎΠ·Π²ΠΎΠ»ΡΡΡΠΈΡ
ΠΈΡ
ΠΏΡΠ΅ΠΎΠ΄ΠΎΠ»Π΅ΡΡ, Ρ Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎΡΡΡΡ Π΄Π°Π»ΡΠ½Π΅ΠΉΡΠ΅ΠΉ ΠΏΡΠΎΡΠ°Π±ΠΎΡΠΊΠΈ Π²ΡΠ±ΡΠ°Π½Π½ΠΎΠ³ΠΎ Π½Π°ΠΏΡΠ°Π²Π»Π΅Π½ΠΈΡ Ρ ΠΏΡΠΈΠ²Π»Π΅ΡΠ΅Π½ΠΈΠ΅ΠΌ Π°Π²ΡΠΎΡΠΈΡΠ΅ΡΠ½ΡΡ
Π½Π°ΡΡΠ½ΡΡ
Π³ΡΡΠΏΠΏ ΠΈ ΠΏΡΠ°ΠΊΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΡΠ΅Π°Π»ΠΈΠ·Π°ΡΠΈΠ΅ΠΉ. ΠΠ°ΡΠ΅ΡΠΈΠ°Π»Ρ ΠΈ ΠΌΠ΅ΡΠΎΠ΄Ρ. ΠΠ°ΡΡΠ½ΡΠΉ Π°Π½Π°Π»ΠΈΠ· Π²ΡΡΠΎΠΊΠΎΠΈΠ½Π΄Π΅ΠΊΡΠΈΡΠΎΠ²Π°Π½Π½ΡΡ
ΠΌΠ΅ΠΆΠ΄ΡΠ½Π°ΡΠΎΠ΄Π½ΡΡ
Π΄ΠΎΠΊΠ»Π°Π΄ΠΎΠ², ΡΡΠ°ΡΠ΅ΠΉ ΠΈ ΠΊΠ»ΠΈΠ½ΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΏΡΠΎΡΠΎΠΊΠΎΠ»ΠΎΠ². Π Π΅Π·ΡΠ»ΡΡΠ°ΡΡ. ΠΡΠ΄Π΅Π»Π΅Π½Ρ ΠΊΡΠΈΡΠΈΡΠ΅ΡΠΊΠΈΠ΅ Π±ΠΈΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΠΌΠ°ΡΠΊΠ΅ΡΡ Π½Π΅Π²ΠΎΡΠΏΡΠΈΠΈΠΌΡΠΈΠ²ΠΎΡΡΠΈ M. tuberculosis ΠΊ ΠΏΡΠΎΡΠΈΠ²ΠΎΡΡΠ±Π΅ΡΠΊΡΠ»Π΅Π·Π½ΠΎΠΉ ΡΠ΅ΡΠ°ΠΏΠΈΠΈ, ΠΊΠΎΡΠΎΡΡΠ΅ Π·Π°ΡΠΈΡΠ°ΡΡ ΠΎΡ ΡΠ°ΡΠΌΠ°ΠΊΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ Π²ΠΌΠ΅ΡΠ°ΡΠ΅Π»ΡΡΡΠ²Π° ΡΠΎ ΡΡΠΎΡΠΎΠ½Ρ ΡΠ΅Π»ΠΎΠ²Π΅ΠΊΠ° ΠΈ Π½Π΅ ΠΏΠΎΠ·Π²ΠΎΠ»ΡΡΡ Π°Π΄Π΅ΠΊΠ²Π°ΡΠ½ΠΎ ΡΠ°Π½ΠΈΡΠΎΠ²Π°ΡΡ ΠΎΡΠ°Π³ΠΈ Π²ΠΎΡΠΏΠ°Π»Π΅Π½ΠΈΡ Π² ΠΎΡΠ³Π°Π½ΠΈΠ·ΠΌΠ΅ Π±ΠΎΠ»ΡΠ½ΠΎΠ³ΠΎ. ΠΡΠ΅Π΄Π»ΠΎΠΆΠ΅Π½Ρ ΡΠΏΠΎΡΠΎΠ±Ρ Π΄Π΅Π·ΠΈΠ½ΡΠ΅Π³ΡΠ°ΡΠΈΠΈ ΠΌΠ΅Ρ
Π°Π½ΠΈΠ·ΠΌΠΎΠ² Π»Π΅ΠΊΠ°ΡΡΡΠ²Π΅Π½Π½ΠΎΠΉ ΡΠ΅Π·ΠΈΡΡΠ΅Π½ΡΠ½ΠΎΡΡΠΈ, ΡΡΠΎ ΠΏΠΎΠ·Π²ΠΎΠ»ΠΈΡ Π²ΡΠ²Π΅ΡΡΠΈ Π°Π»Π³ΠΎΡΠΈΡΠΌΡ Π»Π΅ΡΠ΅Π½ΠΈΡ ΡΡΠ±Π΅ΡΠΊΡΠ»Π΅Π·Π½ΠΎΠΉ ΠΈΠ½ΡΠ΅ΠΊΡΠΈΠΈ Π½Π° Π½ΠΎΠ²ΡΠΉ ΡΡΠΎΠ²Π΅Π½Ρ. ΠΠ°ΠΊΠ»ΡΡΠ΅Π½ΠΈΠ΅. Π‘ ΡΡΠ΅ΡΠΎΠΌ ΠΈΠ·ΡΡΠ΅Π½Π½ΡΡ
ΠΌΠΎΠ»Π΅ΠΊΡΠ»ΡΡΠ½ΡΡ
ΠΈΠ½Π΄ΠΈΠΊΠ°ΡΠΎΡΠΎΠ² ΡΠΎΠΏΡΠΎΡΠΈΠ²Π»ΡΠ΅ΠΌΠΎΡΡΠΈ ΠΊ ΡΡΠ°Π½Π΄Π°ΡΡΠΈΠ·ΠΈΡΠΎΠ²Π°Π½Π½ΡΠΌ ΠΈ ΡΠ°Π·ΡΠ°Π±Π°ΡΡΠ²Π°Π΅ΠΌΡΠΌ Π»Π΅ΠΊΠ°ΡΡΡΠ²Π΅Π½Π½ΡΠΌ ΠΏΡΠ΅ΠΏΠ°ΡΠ°ΡΠ°ΠΌ ΠΏΠΎΠ»ΡΡΠ΅Π½Π½ΡΠ΅ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΡ Π°Π½Π°Π»ΠΈΠ·Π° ΠΈΠ½ΡΠΎΡΠΌΠ°ΡΠΈΠΈ ΠΎ Π²Π°ΠΆΠ½ΠΎΡΡΠΈ ΡΠ΅Π°Π»ΠΈΠ·Π°ΡΠΈΠΈ ΠΏΠ΅ΡΡΠΎΠ½Π°Π»ΠΈΠ·ΠΈΡΠΎΠ²Π°Π½Π½ΠΎΠ³ΠΎ ΠΏΠΎΠ΄Ρ
ΠΎΠ΄Π° Π² ΠΎΠΊΠ°Π·Π°Π½ΠΈΠΈ ΠΌΠ΅Π΄ΠΈΡΠΈΠ½ΡΠΊΠΎΠΉ ΠΏΠΎΠΌΠΎΡΠΈ ΡΡΠΈΠ·ΠΈΠ°ΡΡΠΈΡΠ΅ΡΠΊΠΈΠΌ ΠΏΠ°ΡΠΈΠ΅Π½ΡΠ°ΠΌ ΠΏΠΎΠ·Π²ΠΎΠ»ΡΡ ΡΠ³Π»ΡΠ±ΠΈΡΡ ΠΈ ΡΠ°ΡΡΠΈΡΠΈΡΡ ΠΊΡΡΠ³ΠΎΠ·ΠΎΡ ΡΠΏΠ΅ΡΠΈΠ°Π»ΠΈΡΡΠΎΠ², ΡΡΠ°ΡΡΠ²ΡΡΡΠΈΡ
Π² Π±ΠΎΡΡΠ±Π΅ Ρ ΡΡΠ±Π΅ΡΠΊΡΠ»Π΅Π·ΠΎΠΌ
Radiative Decays of the Upsilon(1S) to a Pair of Charged Hadrons
Using data obtained with the CLEO~III detector, running at the Cornell
Electron Storage Ring (CESR), we report on a new study of exclusive radiative
Upsilon(1S) decays into the final states gamma pi^+ pi^-, gamma K^+ K^-, and
gamma p pbar.. We present branching ratio measurements for the decay modes
Upsilon(1S) to gamma f_2(1270), Upsilon(1S) to gamma f_2'(1525), and
Upsilon(1S) to gamma K^+K^-; helicity production ratios for f_2(1270) and
f_2'(1525); upper limits for the decay Upsilon(1S) to gamma f_J(2200), with
f_J(2220) to pi^+ pi^-, K^+ K^-, p pbar; and an upper limit for the decay
Upsilon(1S) to gamma X(1860), with X(1860) to gamma p pbar.Comment: 17 pages postscript,also available through
http://www.lns.cornell.edu/public/CLNS/2005/, Submitted to PR
Observation of a Narrow Resonance of Mass 2.46 GeV/c^2 Decaying to D_s^*+ pi^0 and Confirmation of the D_sJ^* (2317) State
Using 13.5 inverse fb of e+e- annihilation data collected with the CLEO II
detector we have observed a narrow resonance in the Ds*+pi0 final state, with a
mass near 2.46 GeV. The search for such a state was motivated by the recent
discovery by the BaBar Collaboration of a narrow state at 2.32 GeV, the
DsJ*(2317)+ that decays to Ds+pi0. Reconstructing the Ds+pi0 and Ds*+pi0 final
states in CLEO data, we observe peaks in both of the corresponding
reconstructed mass difference distributions, dM(Dspi0)=M(Dspi0)-M(Ds) and
dM(Ds*pi0)=M(Ds*pi0)-M(Ds*), both of them at values near 350 MeV. We interpret
these peaks as signatures of two distinct states, the DsJ*(2317)+ plus a new
state, designated as the DsJ(2463)+. Because of the similar dM values, each of
these states represents a source of background for the other if photons are
lost, ignored or added. A quantitative accounting of these reflections confirms
that both states exist. We have measured the mean mass differences
= 350.0 +/- 1.2 [stat] +/- 1.0 [syst] MeV for the DsJ*(2317) state, and
= 351.2 +/- 1.7 [stat] +/- 1.0 [syst] MeV for the new DsJ(2463)+
state. We have also searched, but find no evidence, for decays of the two
states via the channels Ds*+gamma, Ds+gamma, and Ds+pi+pi-. The observations of
the two states at 2.32 and 2.46 GeV, in the Ds+pi0 and Ds*+pi0 decay channels
respectively, are consistent with their interpretations as (c anti-strange)
mesons with orbital angular momentum L=1, and spin-parities of 0+ and 1+.Comment: 16 pages postscript, also available through
http://w4.lns.cornell.edu/public/CLNS, version to be published in Physical
Review D; minor modifications and fixes to typographical errors, plus an
added section on production properties. The main results are unchanged; they
supersede those reported in hep-ex/030501
Observation of the ^1P_1 State of Charmonium
The spin-singlet P-wave state of charmonium, hc(1P1), has been observed in
the decay psi(2S) -> pi0 hc followed by hc -> gamma etac. Inclusive and
exclusive analyses of the M(hc) spectrum have been performed. Two complementary
inclusive analyses select either a range of energies for the photon emitted in
hc -> gamma etac or a range of values of M(etac). These analyses, consistent
with one another within statistics, yield M(h_c) =[3524.9 +/- 0.7 (stat) +/-
0.4 (sys)]MeV/c^2 and a product of the branching ratios B_psi(psi(2S) -> pi0
hc) x B_h(hc -> gamma etac) = [3.5 +/- 1.0 (stat) +/- 0.7 (sys)] x 10^{-4}.
When the etac is reconstructed in seven exclusive decay modes, 17.5 +/- 4.5 hc
events are seen with an average mass M(hc) = [3523.6 +/- 0.9 (stat) +/- 0.5
(sys)] MeV/c^2, and B_psi x B_h = [5.3 +/- 1.5 (stat) +/- 1.0 (sys)] x 10^{-4}.
Because the inclusive and exclusive data samples are largely independent they
are combined to yield an overall mass M(hc) = [3524.4 +/- 0.6 (stat) +/- 0.4
(sys)]MeV/c^2 and product of branching ratios B_psi x B_h = [4.0 +/- 0.8 (stat)
+/- 0.7 (sys)] x 10^{-4}. The hc mass implies a P-wave hyperfine splitting
Delta M_{HF}(1P) \equiv M(1^3P)-M(1^1P_1) = [1.0 +/- 0.6 (stat) +/- 0.4 (sys)]
MeV/c^2.Comment: 38 pages postscript,also available through
http://www.lns.cornell.edu/public/CLNS/2005/, Submitted to PR
Search for X(3872) in gamma gamma Fusion and ISR at CLEO
We report on a search for the recently reported X(3872) state using 15.1
fb^{-1} e+ e- data taken in the \sqrt{s} = 9.46-11.30 GeV region. Separate
searches for the production of X(3872) in untagged gamma-gamma fusion and e+ e-
annihilation following initial state radiation (ISR) are made by taking
advantage of the unique correlation of J/psi -> l+ l- in X(3872) decay to pi+
pi- J/psi. No signals are observed in either case, and 90% confidence upper
limits are established as (2J+1)\Gamma_{\gamma\gamma}B(X -> pi+ pi- J/psi) <
12.9 eV and \Gamma_{ee}B(X -> pi+ pi- J/psi) < 8.3 eV.Comment: 8 pages postscript,also available through
http://www.lns.cornell.edu/public/CLNS/2004/, submitted to PR
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