Searches for superparticles at the LHC by application of computer simulation
The analys of recent experimental data received from LHC (CMS) restricts the range of MSSM parameters to the new five parameters. Using computer programs SOFTSUSY, SDECAY and PYTHIA the mass spectrum, partial width and production cross sections of superpatners are calculated. In the context of Minim...
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Obikhod, T.V. Malyuta, Yu.M. 2017-01-15T11:52:19Z 2017-01-15T11:52:19Z 2013 Searches for superparticles at the LHC by application of computer simulation / T.V. Obikhod, Yu.M. Malyuta // Вопросы атомной науки и техники. — 2013. — № 3. — С. 147-150. — Бібліогр.: 10 назв. — англ. 1562-6016 PACS: 11.25.-w, 12.60.Jv, 02.10.Ws https://nasplib.isofts.kiev.ua/handle/123456789/111856 The analys of recent experimental data received from LHC (CMS) restricts the range of MSSM parameters to the new five parameters. Using computer programs SOFTSUSY, SDECAY and PYTHIA the mass spectrum, partial width and production cross sections of superpatners are calculated. In the context of Minimal Supersymmetric Standard Model histograms of mass distributions for superpartners qR and g are constructed. Аналiз останнiх експериментальних даних, отриманих на LHC, обмежив простiр MSSM параметрiв до нових п’яти параметрiв. Шляхом застосування комп’ютерних програм SOFTSUSY, SDECAY i PYTHIA розраховано маси, ширини розпадiв i перерiзи народження суперчастинок. У контекстi мiнiмальної суперсиметричної стандартної моделi побудованi гiстограми розподiлу мас суперчастинок qR и g. Анализ последних экспериментальных данных, полученных на LHC, ограничил пространство MSSM параметров до новых пяти параметров. Путем применения компьютерных программ SOFTSUSY, SDECAY и PYTHIA посчитаны массы, ширины распадов и сечения рождения суперчастиц. В контексте минимальной суперсимметричной стандартной модели построены гистограммы распределения масс суперчастиц qR и g. en Національний науковий центр «Харківський фізико-технічний інститут» НАН України Вопросы атомной науки и техники Ядерная физика и элементарные частицы α Searches for superparticles at the LHC by application of computer simulation Пошуки суперчастинок на LHC шляхом застосування комп’ютерного симулювання Поиски суперчастиц на LHC путем применения компьютерного симулирования Article published earlier |
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| title |
Searches for superparticles at the LHC by application of computer simulation |
| spellingShingle |
Searches for superparticles at the LHC by application of computer simulation Obikhod, T.V. Malyuta, Yu.M. Ядерная физика и элементарные частицы α |
| title_short |
Searches for superparticles at the LHC by application of computer simulation |
| title_full |
Searches for superparticles at the LHC by application of computer simulation |
| title_fullStr |
Searches for superparticles at the LHC by application of computer simulation |
| title_full_unstemmed |
Searches for superparticles at the LHC by application of computer simulation |
| title_sort |
searches for superparticles at the lhc by application of computer simulation |
| author |
Obikhod, T.V. Malyuta, Yu.M. |
| author_facet |
Obikhod, T.V. Malyuta, Yu.M. |
| topic |
Ядерная физика и элементарные частицы α |
| topic_facet |
Ядерная физика и элементарные частицы α |
| publishDate |
2013 |
| language |
English |
| container_title |
Вопросы атомной науки и техники |
| publisher |
Національний науковий центр «Харківський фізико-технічний інститут» НАН України |
| format |
Article |
| title_alt |
Пошуки суперчастинок на LHC шляхом застосування комп’ютерного симулювання Поиски суперчастиц на LHC путем применения компьютерного симулирования |
| description |
The analys of recent experimental data received from LHC (CMS) restricts the range of MSSM parameters to the new five parameters. Using computer programs SOFTSUSY, SDECAY and PYTHIA the mass spectrum, partial width and production cross sections of superpatners are calculated. In the context of Minimal Supersymmetric Standard Model histograms of mass distributions for superpartners qR and g are constructed.
Аналiз останнiх експериментальних даних, отриманих на LHC, обмежив простiр MSSM параметрiв до нових п’яти параметрiв. Шляхом застосування комп’ютерних програм SOFTSUSY, SDECAY i PYTHIA розраховано маси, ширини розпадiв i перерiзи народження суперчастинок. У контекстi мiнiмальної суперсиметричної стандартної моделi побудованi гiстограми розподiлу мас суперчастинок qR и g.
Анализ последних экспериментальных данных, полученных на LHC, ограничил пространство MSSM параметров до новых пяти параметров. Путем применения компьютерных программ SOFTSUSY, SDECAY и PYTHIA посчитаны массы, ширины распадов и сечения рождения суперчастиц. В контексте минимальной суперсимметричной стандартной модели построены гистограммы распределения масс суперчастиц qR и g.
|
| issn |
1562-6016 |
| url |
https://nasplib.isofts.kiev.ua/handle/123456789/111856 |
| citation_txt |
Searches for superparticles at the LHC by application of computer simulation / T.V. Obikhod, Yu.M. Malyuta // Вопросы атомной науки и техники. — 2013. — № 3. — С. 147-150. — Бібліогр.: 10 назв. — англ. |
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| fulltext |
SEARCHES FOR SUPERPARTICLES AT THE LHC BY
APPLICATION OF COMPUTER SIMULATION
T.V. Obikhod ∗, Yu.M. Malyuta
Institute for Nuclear Research, NAS of Ukraine 03680 Kiev, Ukraine
(Received February 6, 2012)
The analys of recent experimental data received from LHC (CMS) restricts the range of MSSM parameters to the new
five parameters. Using computer programs SOFTSUSY, SDECAY and PYTHIA the mass spectrum, partial width
and production cross sections of superpatners are calculated. In the context of Minimal Supersymmetric Standard
Model histograms of mass distributions for superpartners q̃R and g̃ are constructed.
PACS: 11.25.-w, 12.60.Jv, 02.10.Ws
1. INTRODUCTION
The searches for new physics at the LHC moti-
vated the necessary tools for building Grand Uni-
fication Theory (GUT) models in F-theory [1]. It
is known that Minimal Supersymmetric Standard
Model (MSSM) [2] through its connection to string
theory improves the Standard Model (SM). There are
several problems of SM, connected with our experi-
mental knowledge and with some theoretical aspects:
1) there is the neutrino mass problem - the SM
predicts neutrinos having zero mass, whereas we have
experimental evidence for massive neutrinos;
2) SM field theory which include gravity ends up
being non-renormalizable without predictions below
the Planck scale;
3) SM has 19 free parameters to be determined
experimentally;
4) the hierarchy problem;
5) the unification problem.
These problems can be decided with the help of
MSSM model. In this model each particle, for ex-
ample fermion, has its superpartner - boson with ap-
propriate masses and couplings. MSSM includes new
symmetry called R-parity. This gives us some usefull
phenomenological results:
• the lightest sparticle, LSP must be stable and
than it would be an excellent candidate for dark mat-
ter;
• the LSP interacts very weakly with matter;
• supersymmetric particles are produced in pairs;
• all supersymmetric particles are unstable and
decay.
2. CATEGORY OF D-BRANES
To construct the MSSM model from superstring the-
ory we must use the notion of derived category [3].
We will give the short review of the theory of cate-
gory.
A category L consists of the following data:
1) A class Ob L of objects A,B, C, · · · ;
2) A family of disjoint sets of morphisms
Hom(A,B) one for each ordered pair A,B of
objects;
3) A family of maps
Hom(A, B)×Hom(B, C) → Hom(A,C) ,
one for each ordered triplet A,B, C of objects.
These data obey the axioms:
a) If f : A → B, g : B → C, h : C → D,
then composition of morphisms is associative, that
is, h(gf) = (hg)f ;
b) To each object B there exists a morphism
1B : B → B such that 1Bf = f , g1B = g for
f : A → B and g : B → C .
There are several aspects that are necessary for con-
struction the category of D-branes [3]:
• D-brane is associated to the locally-free sheaf;
• An open string from one D-brane (sheaf E) to
another D-brane (sheaf F ) is given by an element of
the group Extq(E, F ) ;
• the category of D-branes is the derived category
of coherent sheaves D(X) ;
• If X and Y are mirror Calabi-Yau threefolds
then the category D(X) is equivalent to the triangu-
lated category TrF(Y ) ;
• D-branes on the orbifold C/G and open strings
between them are described by the derived category
of McKay quiver representations.
We consider the derived category of distinguished tri-
angles over the abelian category of McKay quivers [?].
Objects of this category are distinguished triangles
∗Corresponding author E-mail address: obikhod@kinr.kiev.ua
ISSN 1562-6016. PROBLEMS OF ATOMIC SCIENCE AND TECHNOLOGY, 2013, N3(85).
Series: Nuclear Physics Investigations (60), p.147-150.
147
Fig.1. Triangles
(numbers a, b, c and a′, b′, c′ denote orbifold charges
[4] characterizing McKay quivers); morphisms of this
category are morphisms of distinguished triangles.
3. PARTICLE CONTENT
The moduli space of an open superstring [5] has the
form
Ext0(Q,Q
′
) = C aa
′
+bb
′
+cc
′
,
Ext1(Q,Q
′
) = C 3ab
′
+3bc
′
+3ca
′
.
(1)
Substituting in (1) orbifold charges
a = b = c = a′ = b′ = c′ = 4
(Fig. 1) and using the Langlands hypothesis [6], we
obtain the realization of (1) in terms of SU(5) mul-
tiplets
3× (24 + 5H + 5H + 5M + 5M + 10M + 10M ) .
This result determines the particle content of the
MSSM.
4. SUPERPOTENTIAL
The gauge invariant MSSM superpotential takes the
form
WSU(5) = λd
ij · 5H × 5(i)
M × 10(j)
M +
+λu
ij · 5H × 10(i)
M × 10(j)
M + µ · 5H × 5H ,
(2)
where 5H and 5H are Higgs multiplets, 5(i)
M and 10(j)
M
are multiplets of quark and lepton superpartners,
λd
ij , λu
ij are Yukawa coupling constants and µ is the
Higgs mixing parameter.
5. MASS SPECTRUM
The analysis of Yukawa coupling constants, based on
observational hints and theoretical considerations, al-
lows to restrict the parameter space in (2) to five free
parameters [7]:
M0 = 450 GeV , M1/2 = 425 GeV ,
A0 = 0 , tanβ = 10 , sgn(µ) = +1 .
(3)
Using this restricted parameter set it is possible to
calculate the mass spectrum of superpartners by
application of the computer program SOFTSUSY
[8]. This MSSM spectrum is shown in Table 1.
Table 1. Mass spectrum of superpartners
GeV GeV GeV
ũR 974 g̃ 1006
ũL 1000 ν̃e 525 χ̃0
1 174
d̃R 972 ẽR 477 χ̃0
2 327
d̃L 1003 ẽL 531 χ̃0
3 546
c̃R 974 χ̃0
4 562
c̃L 1000 ν̃µ 525 χ̃±1 327
s̃R 972 µ̃R 477 χ̃±2 562
s̃L 1003 µ̃L 531
t̃1 741 h0 114
t̃2 947 ν̃τ 523 A0 749
b̃1 910 τ̃1 471 H0 749
b̃2 968 τ̃2 531 H± 753
6. PARTIAL WIDTHS
Using the parameter set (3) it is possible to calcu-
late partial widths of superpartners by application of
the computer program SDECAY [9]. These partial
widths are shown in Tables 2, 3.
Table 2. Partial widths of superpartners
channel BR channel BR
ũR χ̃0
1u 0.993 χ̃0
4u 0.004
χ̃0
2u 0.002
d̃R χ̃0
1d 0.993 χ̃0
4d 0.004
χ̃0
2d 0.002
c̃R χ̃0
1c 0.993 χ̃0
4c 0.004
χ̃0
2c 0.002
s̃R χ̃0
1s 0.993 χ̃0
4s 0.004
χ̃0
2s 0.002
Table 3. Partial widths of superpartners
channel BR channel BR
g̃ d̃Rd∗ 0.017 b̃1b
∗ 0.119
d̃∗Rd 0.017 b̃∗1b 0.119
ũRu∗ 0.015 b̃2b
∗ 0.021
ũ∗Ru 0.015 b̃∗2b 0.021
s̃Rs∗ 0.017 t̃1t
∗ 0.294
s̃∗Rs 0.017 t̃∗1t 0.294
c̃Rc∗ 0.015
c̃∗Rc 0.015
7. CROSS SECTIONS
Using the parameter set (3) it is possible to calculate
production cross sections of superpartners by appli-
cation of the computer program PYTHIA [10]. These
cross sections at center-of-mass energy
√
s = 14 TeV
are shown in Table 4.
148
Table 4. Cross sections of superpartners
channel cross section, pb
gg → g̃g̃ σg̃g̃ = 0.323
qg → d̃Rg̃ σd̃Rg̃ = 0.260
qg → ũRg̃ σũRg̃ = 0.489
qq
′ → ũRd̃R σũRd̃R
= 0.132
8. RECONSTRUCTION OF MASSES
To construct histograms describing mass distribu-
tions for superpartners q̃R and g̃ we choose the set of
parameters (3). Using this parameter set it is possible
to construct histograms of mass distributions for su-
perpartners by application of the computer program
PYTHIA [10]. This histograms are shown in Fig. 2
and Fig. 3.
Fig.2. Histogram of mass distribution for q̃R Fig.3. Histogram of mass distribution for g̃
References
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9. M. Muhlleitner, A. Djouadi and Y. Mambrini.
SDECAY: a fortran code for the decays of the
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149
ПОИСКИ СУПЕРЧАСТИЦ НА LHC ПУТЕМ ПРИМЕНЕНИЯ КОМПЬЮТЕРНОГО
СИМУЛИРОВАНИЯ
Т.В.Обиход, Ю.М.Малюта
Анализ последних экспериментальных данных, полученных на LHC, ограничил пространство MSSM
параметров до новых пяти параметров. Путем применения компьютерных программ SOFTSUSY, SDECAY
и PYTHIA посчитаны массы, ширины распадов и сечения рождения суперчастиц. В контексте мини-
мальной суперсимметричной стандартной модели построены гистограммы распределения масс супер-
частиц q̃R и g̃.
ПОШУКИ СУПЕРЧАСТИНОК НА LHC ШЛЯХОМ ЗАСТОСУВАННЯ
КОМП’ЮТЕРНОГО СИМУЛЮВАННЯ
Т.В.Обiход, Ю.М.Малюта
Аналiз останнiх експериментальних даних, отриманих на LHC, обмежив простiр MSSM параметрiв до
нових п’яти параметрiв. Шляхом застосування комп’ютерних програм SOFTSUSY, SDECAY i PYTHIA
розраховано маси, ширини розпадiв i перерiзи народження суперчастинок. У контекстi мiнiмальної су-
персиметричної стандартної моделi побудованi гiстограми розподiлу мас суперчастинок q̃R и g̃.
150
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