421 research outputs found
The lithium stellarator experiment. TJ-II as a benchmark
In the last years, lithium wall conditioning has been carried out in several fusion devices (Tokamaks, Compact Toruses) by different techniques, providing in many instances record values of plasma parameters and enhanced plasma reproducibility. Behind these findings are the low recycling, low contamination and non-coronal enhanced radiative power dissipation properties of Li. Stellarators are best suited for reactor concepts as far as they basically free from extreme thermal load events. However, the potential problem of impurity accumulation must be taken into account. Therefore, the use of low Z elements as PFC would be highly desirable. In the present work, the plasma performance of the TJ-II Heliac under Li-coated wall conditions with lithium is described. Compared to previous coatings, lithium has produced the best plasma performance to date, leading to the achievement of record values in plasma density and energy confinement. In the present work, the impact of the Li coating operation on reactor relevant issues, such as particle exhaust and retention, high-density operation, confinement characteristics and plasma wall interaction issues is stressed.На протязі останніх років обробку стінок літієм було проведено в кількох термоядерних установках (токамаки, компактні тори) з використанням різних методів, що забезпечило у багатьох випадках одержання плазми з рекордними параметрами та покращеним відтворенням результатів. Ці результати пов’язані з низьким рециклінгом, що властивий літію, слабким забрудненням плазми і підвищеним не корональним поглинанням випромінювання. Стеларатори краще за все підходять для концепції реактора, бо в них у принципі не може бути підвищених теплових навантажень. Але треба враховувати можливість накопичення домішок. Тому конче бажано в поверхнях, які повернені до плазми, використовувати елементи з низьким Z. В даній роботі описано експерименти по одержанню плазми в геліаку TJ-II в умовах покриття стінок літієм. Порівняно з покриттями, що використовувалися раніше, літій забезпечив одержання плазми з найкращими на даний час параметрами, дозволивши досягти рекордних значень гущини плазми та утримання енергії. Підкреслена важливість літієвого покриття для таких аспектів реактора, як втрати і затримування частинок, робота при високій гущині, характеристики утримання та взаємодія плазма-стінка.В течение последних лет обработка стенок литием была проведена в нескольких термоядерных установках (токамаки, компактные торы) с использованием различных методов, что обеспечило во многих случаях получение плазмы с рекордными параметрами и улучшенной воспроизводимостью результатов. Эти результаты связаны со свойственными литию низким рециклингом, слабым загрязнением плазмы и повышенным не корональным поглощением излучения. Стеллараторы лучше всего подходят для концепции реактора, ибо у них в принципе не может быть повышенных тепловых нагрузок. Однако, необходимо учитывать возможность накопления примесей. Поэтому весьма желательно в поверхностях, обращённых к плазме, использовать элементы с низким Z. В настоящей работе описаны эксперименты по получению плазмы в гелиаке TJ-II в условиях покрытия стенок литием. По сравнению с покрытиями, которые использовались раньше, литий обеспечил получение плазмы с наилучшими в настоящее время параметрами, позволив достичь рекордных значений плотности плазмы и удержания энергии. Подчёркивается важность литиевого покрытия для таких аспектов реактора, как расход и удерживание частиц, работа при большой плотности, характеристики удержания и взаимодействие плазма-стенка
Investigation of plasma turbulence and local electric field in the T-10 tokamak and TJ-II stellarator by HIBP diagnoatic(review)
TJ-II stellarator by HIBP diagnostics has been performed. The following similar features of potential were found: the
scale of several hundred Volts; the negative sign for densities ne>1×10¹⁹ m⁻³ and comparable values in spite of the
different heating methods. When ne or tE rises, the potential evolves to negative values. During ECR heating and
associated Te rise, tE degrades and the potential evolves to positive direction. Oscillations of potential and density in the
range of Geodesic Acoustic Modes in T-10 and Alfvén Eigenmodes in TJ-II were observed.На токамаці Т-10 і стелараторі TJ-II за допомогою пучка важких іонів в порівняних режимах досліджувалася поведінка потенціалу та його флуктуацій. Виявлені спільні властивості потенціалу: масштаб близько сотен вольт;негативний знак при щільності ne>1×10¹⁹ m⁻³ і порівнянні значення, незважаючи на різні методи нагріву. Коли n_е або t_Е зростають, потенціал зростае у негативну область. При ЕЦР-нагріві і відповідному рості Te, t_Е погіршується, і потенціал змінюється у позитивний бік. Спостерігається коливання потенціалу в діапазоні геодезичних акустичних мод у Т-10 та альфвеновських власних мод у TJ-IIНа токамаке Т-10 и стеллараторе TJ-II с помощью пучка тяжелых ионов в сравнимых режимах исследовалось поведение потенциала и его флуктуаций. Обнаружены общие свойства потенциала: масштаб порядка сотен вольт; отрицательный знак при плотностях
n_е>1×10¹⁹ m⁻³ и сравнимые значения, несмотря на разные методы нагрева. Когда n_е или t_Е растут, потенциал растет в отрицательную область. При ЭЦР-нагреве и соответствующем росте Te, t_Е ухудшается, и потенциал меняется в положительную сторону. Наблюдались колебания потенциала в диапазоне геодезических акустических мод в Т-10 и альфвеновских собственных мод в TJ-I
Measurement of Z/gamma*+jet+X angular distributions in ppbar collisions at sqrt{s}=1.96 TeV
We present the first measurements at a hadron collider of differential cross
sections for Z+jet+X production in delta phi(Z, jet), |delta y(Z, jet)| and
|y_boost(Z, jet)|. Vector boson production in association with jets is an
excellent probe of QCD and constitutes the main background to many small cross
section processes, such as associated Higgs production. These measurements are
crucial tests of the predictions of perturbative QCD and current event
generators, which have varied success in describing the data. Using these
measurements as inputs in tuning event generators will increase the
experimental sensitivity to rare signals.Comment: Published in Physics Letters B 682 (2010), pp. 370-380. 15 pages, 6
figure
Search for the standard model Higgs boson in tau final states
We present a search for the standard model Higgs boson using hadronically
decaying tau leptons, in 1 inverse femtobarn of data collected with the D0
detector at the Fermilab Tevatron ppbar collider. We select two final states:
tau plus missing transverse energy and b jets, and tau+ tau- plus jets. These
final states are sensitive to a combination of associated W/Z boson plus Higgs
boson, vector boson fusion and gluon-gluon fusion production processes. The
observed ratio of the combined limit on the Higgs production cross section at
the 95% C.L. to the standard model expectation is 29 for a Higgs boson mass of
115 GeV.Comment: publication versio
Search for charged Higgs bosons in top quark decays
We present a search for charged Higgs bosons in top quark decays. We analyze
the \eplus, \muplus, , , , \etau and \mutau final states from
top quark pair production events, using data from about 1 of
integrated luminosity recorded by the \dzero experiment at the Fermilab
Tevatron Collider. We consider different scenarios of possible charged Higgs
boson decays, one where the charged Higgs boson decays purely hadronically into
a charm and a strange quark, another where it decays into a lepton and a
neutrino and a third one where both decays appear. We extract limits on
the branching ratio for all these models. We use two methods,
one where the production cross section is fixed, and one where the
cross section is fitted simultaneously with . Based on the
extracted limits, we exclude regions in the charged Higgs boson mass and parameter space for different scenarios of the minimal supersymmetric
standard model.Comment: 10 pages, 8 figures, submitted to PL
Search for W' bosons decaying to an electron and a neutrino with the D0 detector
This Letter describes the search for a new heavy charged gauge boson W'
decaying into an electron and a neutrino. The data were collected with the D0
detector at the Fermilab Tevatron proton-antiproton Collider at a
center-of-mass energy of 1.96 TeV, and correspond to an integrated luminosity
of about 1 inverse femtobarn. Lacking any significant excess in the data in
comparison with known processes, an upper limit is set on the production cross
section times branching fraction, and a W' boson with mass below 1.00 TeV can
be excluded at the 95% C.L., assuming standard-model-like couplings to
fermions. This result significantly improves upon previous limits, and is the
most stringent to date.Comment: submitted to Phys. Rev. Let
Search for a scalar or vector particle decaying into Zgamma in ppbar collisions at sqrt(s) = 1.96 TeV
We present a search for a narrow scalar or vector resonance decaying into
Zgamma with a subsequent Z decay into a pair of electrons or muons. The data
for this search were collected with the D0 detector at the Fermilab Tevatron
ppbar collider at a center of mass energy sqrt(s) = 1.96 TeV. Using 1.1 (1.0)
fb-1 of data, we observe 49 (50) candidate events in the electron (muon)
channel, in good agreement with the standard model prediction. From the
combination of both channels, we derive 95% C.L. upper limits on the cross
section times branching fraction (sigma x B) into Zgamma. These limits range
from 0.19 (0.20) pb for a scalar (vector) resonance mass of 600 GeV/c^2 to 2.5
(3.1) pb for a mass of 140 GeV/c^2.Comment: Published by Phys. Lett.
Search for a W' boson decaying to a bottom quark and a top quark in pp collisions at sqrt(s) = 7 TeV
Results are presented from a search for a W' boson using a dataset
corresponding to 5.0 inverse femtobarns of integrated luminosity collected
during 2011 by the CMS experiment at the LHC in pp collisions at sqrt(s)=7 TeV.
The W' boson is modeled as a heavy W boson, but different scenarios for the
couplings to fermions are considered, involving both left-handed and
right-handed chiral projections of the fermions, as well as an arbitrary
mixture of the two. The search is performed in the decay channel W' to t b,
leading to a final state signature with a single lepton (e, mu), missing
transverse energy, and jets, at least one of which is tagged as a b-jet. A W'
boson that couples to fermions with the same coupling constant as the W, but to
the right-handed rather than left-handed chiral projections, is excluded for
masses below 1.85 TeV at the 95% confidence level. For the first time using LHC
data, constraints on the W' gauge coupling for a set of left- and right-handed
coupling combinations have been placed. These results represent a significant
improvement over previously published limits.Comment: Submitted to Physics Letters B. Replaced with version publishe
Search for the standard model Higgs boson decaying into two photons in pp collisions at sqrt(s)=7 TeV
A search for a Higgs boson decaying into two photons is described. The
analysis is performed using a dataset recorded by the CMS experiment at the LHC
from pp collisions at a centre-of-mass energy of 7 TeV, which corresponds to an
integrated luminosity of 4.8 inverse femtobarns. Limits are set on the cross
section of the standard model Higgs boson decaying to two photons. The expected
exclusion limit at 95% confidence level is between 1.4 and 2.4 times the
standard model cross section in the mass range between 110 and 150 GeV. The
analysis of the data excludes, at 95% confidence level, the standard model
Higgs boson decaying into two photons in the mass range 128 to 132 GeV. The
largest excess of events above the expected standard model background is
observed for a Higgs boson mass hypothesis of 124 GeV with a local significance
of 3.1 sigma. The global significance of observing an excess with a local
significance greater than 3.1 sigma anywhere in the search range 110-150 GeV is
estimated to be 1.8 sigma. More data are required to ascertain the origin of
this excess.Comment: Submitted to Physics Letters
Measurement of the Lambda(b) cross section and the anti-Lambda(b) to Lambda(b) ratio with Lambda(b) to J/Psi Lambda decays in pp collisions at sqrt(s) = 7 TeV
The Lambda(b) differential production cross section and the cross section
ratio anti-Lambda(b)/Lambda(b) are measured as functions of transverse momentum
pt(Lambda(b)) and rapidity abs(y(Lambda(b))) in pp collisions at sqrt(s) = 7
TeV using data collected by the CMS experiment at the LHC. The measurements are
based on Lambda(b) decays reconstructed in the exclusive final state J/Psi
Lambda, with the subsequent decays J/Psi to an opposite-sign muon pair and
Lambda to proton pion, using a data sample corresponding to an integrated
luminosity of 1.9 inverse femtobarns. The product of the cross section times
the branching ratio for Lambda(b) to J/Psi Lambda versus pt(Lambda(b)) falls
faster than that of b mesons. The measured value of the cross section times the
branching ratio for pt(Lambda(b)) > 10 GeV and abs(y(Lambda(b))) < 2.0 is 1.06
+/- 0.06 +/- 0.12 nb, and the integrated cross section ratio for
anti-Lambda(b)/Lambda(b) is 1.02 +/- 0.07 +/- 0.09, where the uncertainties are
statistical and systematic, respectively.Comment: Submitted to Physics Letters
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