SUSYCrossSections13TeVhinosplit < LHCPhysics

---+ NLO-NLL Higgsino-like Cross Sections (non-fully-degenerate case)

The following cross sections are for pure higgsino-like pair production. They differ from the [[SUSYCrossSections13TeVhino][fully-degenerate case]] because here not all of the higgsinos are assumed to have the same mass, but there is a mass splitting between the two lightest neutralinos of <latex>\Delta M = m(\tilde\chi_2^0) - m(\tilde\chi_1^0)</latex>, and the mass of the lighter chargino is half-way in between the two neutralinos, <latex>m(\tilde\chi^\pm_1) = m(\tilde\chi_1^0) + \Delta M/2</latex>. 
These NLO+NLL cross-sections were computed using Resummino and an envelope of the CTEQ6.6 and MSTW2008nlo90cl PDFs.
In addition, a dedicated calculation of the branching ratios (BR) of the <latex>\tilde\chi_2^0</latex> into two leptons and the <latex>\tilde\chi_1^\pm</latex> into a lepton and neutrino (including the tau lepton(s) where possible) was done with SUSYHit. 
In this calculation the decays of <latex>\tilde\chi_2^0</latex> into <latex>\tilde\chi_1^\pm + X</latex> or <latex>\tilde\chi_1^0 + \gamma</latex> are not allowed.
The values are listed in the tables below.

When using these cross sections, please cite the following two references, available below in bibtex format:

%TWISTY{mode="div" showlink="Show References " hidelink="Hide References " firststart="hide" showimgright="%ICONURLPATH{toggleopen-small}%" hideimgright="%ICONURLPATH{toggleclose-small}%"}%
<verbatim>

@article{Fuks:2012qx,
      author         = "Fuks, Benjamin and Klasen, Michael and Lamprea, David R.
                        and Rothering, Marcel",
      title          = "{Gaugino production in proton-proton collisions at a
                        center-of-mass energy of 8 TeV}",
      journal        = "JHEP",
      volume         = "10",
      pages          = "081",
      doi            = "10.1007/JHEP10(2012)081",
      year           = "2012",
      eprint         = "1207.2159",
      archivePrefix  = "arXiv",
      primaryClass   = "hep-ph",
      reportNumber   = "IPHC-PHENO-12-07, MS-TP-12-05",
      SLACcitation   = "%%CITATION = ARXIV:1207.2159;%%",
}

@article{Fuks:2013vua,
      author         = "Fuks, Benjamin and Klasen, Michael and Lamprea, David R.
                        and Rothering, Marcel",
      title          = "{Precision predictions for electroweak superpartner
                        production at hadron colliders with {\sc Resummino}}",
      journal        = "Eur. Phys. J. C",
      volume         = "73",
      pages          = "2480",
      doi            = "10.1140/epjc/s10052-013-2480-0",
      year           = "2013",
      eprint         = "1304.0790",
      archivePrefix  = "arXiv",
      primaryClass   = "hep-ph",
      reportNumber   = "CERN-PH-TH-2013-064, IPHC-PHENO-13-02, MS-TP-13-06",
      SLACcitation   = "%%CITATION = ARXIV:1304.0790;%%",
}</verbatim>
%ENDTWISTY%

Two SLHA templates are attached that have been used in the cross-section calculations:
   * !N2N1, !N2C1p, !N2C1m: [[%ATTACHURL%/higgsino_slha.in][higgsino_slha.in]]
   * !C1C1: [[%ATTACHURL%/higgsino_slha_C1C1.in][higgsino_slha_C1C1.in]] (Technical remark: The masses of some of the decoupled !SUSY particles are set to less extreme (i.e. somewhat lower) mass values in this SLHA file to avoid crashes in loop calculations.)

<!-- ---++ NLO-NLL hino-like &chi;&#x303;&chi;&#x303; -->
---+++ !C1pN2 (<latex>\tilde\chi_1^+ \tilde\chi_2^0</latex>) Higgsino production 
%TWISTY{mode="div" showlink="Show table " hidelink="Hide table " firststart="hide" showimgright="%ICONURLPATH{toggleopen-small}%" hideimgright="%ICONURLPATH{toggleclose-small}%" remember="on"}%
|<latex>m(\tilde\chi_2^0)</latex> [GeV] | <latex>m(\tilde\chi_1^\pm)</latex> [GeV] | <latex>m(\tilde\chi_1^0)</latex> [GeV] |  xsec [pb]  |  relative uncertainty  |				
|100|80|60|5.00771|0.02106|
|120|90|60|2.83624|0.02290|
|81.5|80.75|80|7.47073|0.01914|
|82|81|80|7.34199|0.01992|
|83|81.5|80|7.08993|0.02006|
|85|82.5|80|6.62058|0.02022|
|90|85|80|5.61532|0.02072|
|95|87.5|80|4.80271|0.02120|
|100|90|80|4.13934|0.02170|
|110|95|80|3.13403|0.02266|
|120|100|80|2.42578|0.02363|
|140|110|80|1.53031|0.02552|
|101.5|100.75|100|3.30590|0.02181|
|102|101|100|3.26241|0.02254|
|103|101.5|100|3.17638|0.02264|
|105|102.5|100|3.01358|0.02279|
|110|105|100|2.65145|0.02327|
|115|107.5|100|2.34357|0.02378|
|120|110|100|2.08078|0.02425|
|130|115|100|1.65896|0.02520|
|140|120|100|1.34117|0.02615|
|160|130|100|0.90709|0.02798|
|126.5|125.75|125|1.50030|0.02484|
|127|126|125|1.48393|0.02570|
|128|126.5|125|1.45393|0.02579|
|130|127.5|125|1.39465|0.02598|
|135|130|125|1.25940|0.02644|
|140|132.5|125|1.14041|0.02690|
|145|135|125|1.03536|0.02736|
|155|140|125|0.85959|0.02827|
|165|145|125|0.71995|0.02917|
|185|155|125|0.51616|0.03096|
|152|151|150|0.78365|0.02876|
|153|151.5|150|0.76995|0.02887|
|155|152.5|150|0.74360|0.02903|
|160|155|150|0.68252|0.02947|
|165|157.5|150|0.62755|0.02991|
|170|160|150|0.57814|0.03036|
|180|165|150|0.49299|0.03123|
|190|170|150|0.42304|0.03210|
|210|180|150|0.31662|0.03381|
|178|176.5|175|0.44809|0.03085|
|180|177.5|175|0.43479|0.03104|
|185|180|175|0.40360|0.03146|
|190|182.5|175|0.37514|0.03189|
|195|185|175|0.34914|0.03231|
|202|201|200|0.28275|0.03454|
|203|201.5|200|0.27896|0.03458|
|205|202.5|200|0.27160|0.03479|
|210|205|200|0.25423|0.03520|
|215|207.5|200|0.23820|0.03561|
|220|210|200|0.22341|0.03603|
|230|215|200|0.19674|0.03683|
|240|220|200|0.17444|0.03765|
|260|230|200|0.13801|0.03924|
|230|227.5|225|0.17820|0.03663|
|235|230|225|0.16787|0.03704|
|240|232.5|225|0.15826|0.03743|
|252|251|250|0.12566|0.03992|
|253|251.5|250|0.12428|0.03997|
|255|252.5|250|0.12157|0.04015|
|260|255|250|0.11511|0.04054|
|265|257.5|250|0.10884|0.04089|
|270|260|250|0.10339|0.04131|
|280|265|250|0.09289|0.04203|
|290|270|250|0.08400|0.04283|
|310|280|250|0.06884|0.04431|
|302|301|300|0.06350|0.04495|
|303|301.5|300|0.06290|0.04502|
|305|302.5|300|0.06172|0.04517|
|310|305|300|0.05888|0.04553|
|315|307.5|300|0.05606|0.04593|
|320|310|300|0.05366|0.04625|
| special masses |||||
|120|105|100|2.24473|0.02393|
|120|115|100|1.92858|0.02456|
|120|120|100|1.78996|0.02488|
|160|152.5|150|0.70118|0.02934|
|160|157.5|150|0.66301|0.02963|
|160|160|150|0.64482|0.02978|
%ENDTWISTY%

---+++ !C1mN2 (<latex>\tilde\chi_1^- \tilde\chi_2^0</latex>) Higgsino production 
%TWISTY{mode="div" showlink="Show table " hidelink="Hide table " firststart="hide" showimgright="%ICONURLPATH{toggleopen-small}%" hideimgright="%ICONURLPATH{toggleclose-small}%" remember="on"}%
|  <latex>m(\tilde\chi_2^0)</latex> [GeV] | <latex>m(\tilde\chi_1^\pm)</latex> [GeV] | <latex>m(\tilde\chi_1^0)</latex> [GeV] |  xsec [pb]  |  relative uncertainty  |
|100|80|60|3.20454|0.04146|
|120|90|60|1.76639|0.04383|
|81.5|80.75|80|4.86322|0.03940|
|82|81|80|4.77871|0.04012|
|83|81.5|80|4.60766|0.04015|
|85|82.5|80|4.28971|0.04049|
|90|85|80|3.61176|0.04109|
|95|87.5|80|3.06705|0.04170|
|100|90|80|2.62492|0.04227|
|110|95|80|1.96067|0.04343|
|120|100|80|1.49791|0.04452|
|140|110|80|0.92186|0.04664|
|101.5|100.75|100|2.07213|0.04294|
|102|101|100|2.04474|0.04326|
|103|101.5|100|1.98820|0.04338|
|105|102.5|100|1.88132|0.04361|
|110|105|100|1.64452|0.04419|
|110|105|100|1.64371|0.04410|
|115|107.5|100|1.44431|0.04472|
|120|110|100|1.27430|0.04529|
|130|115|100|1.00358|0.04630|
|140|120|100|0.80173|0.04728|
|160|130|100|0.52999|0.04925|
|126.5|125.75|125|0.90218|0.04670|
|127|126|125|0.89246|0.04680|
|128|126.5|125|0.87300|0.04695|
|130|127.5|125|0.83544|0.04715|
|135|130|125|0.75003|0.04765|
|140|132.5|125|0.67527|0.04815|
|145|135|125|0.60959|0.04863|
|155|140|125|0.50049|0.04957|
|165|145|125|0.41465|0.05049|
|185|155|125|0.29122|0.05226|
|152|151|150|0.45364|0.05006|
|153|151.5|150|0.44524|0.05020|
|155|152.5|150|0.42907|0.05033|
|160|155|150|0.39173|0.05078|
|165|157.5|150|0.35829|0.05123|
|170|160|150|0.32836|0.05166|
|180|165|150|0.27714|0.05252|
|190|170|150|0.23543|0.05334|
|210|180|150|0.17280|0.05492|
|178|176.5|175|0.25022|0.05271|
|180|177.5|175|0.24231|0.05292|
|185|180|175|0.22381|0.05330|
|190|182.5|175|0.20701|0.05368|
|195|185|175|0.19173|0.05407|
|202|201|200|0.15307|0.05557|
|203|201.5|200|0.15089|0.05558|
|205|202.5|200|0.14663|0.05579|
|210|205|200|0.13661|0.05616|
|215|207.5|200|0.12741|0.05652|
|220|210|200|0.11895|0.05688|
|230|215|200|0.10383|0.05751|
|240|220|200|0.09123|0.05825|
|260|230|200|0.07093|0.05955|
|230|227.5|225|0.09328|0.05768|
|235|230|225|0.08749|0.05800|
|240|232.5|225|0.08212|0.05834|
|252|251|250|0.06412|0.06009|
|253|251.5|250|0.06336|0.06007|
|255|252.5|250|0.06188|0.06027|
|260|255|250|0.05834|0.06058|
|265|257.5|250|0.05493|0.06077|
|270|260|250|0.05197|0.06118|
|280|265|250|0.04631|0.06169|
|290|270|250|0.04155|0.06233|
|310|280|250|0.03352|0.06344|
|302|301|300|0.03072|0.06391|
|303|301.5|300|0.03040|0.06396|
|305|302.5|300|0.02979|0.06407|
|310|305|300|0.02831|0.06433|
|315|307.5|300|0.02684|0.06467|
|320|310|300|0.02561|0.06485|
| special masses |||||
|120|105|100|1.38092|0.04493|
|120|115|100|1.17681|0.04565|
|120|120|100|1.08784|0.04601|
|160|152.5|150|0.40332|0.05067|
|160|157.5|150|0.38002|0.05096|
|160|160|150|0.36894|0.05110|
%ENDTWISTY%

---+++ !N2N1 (<latex>\tilde\chi_2^0 \tilde\chi_1^0</latex>) Higgsino production 
%TWISTY{mode="div" showlink="Show table " hidelink="Hide table " firststart="hide" showimgright="%ICONURLPATH{toggleopen-small}%" hideimgright="%ICONURLPATH{toggleclose-small}%" remember="on"}%
|  <latex>m(\tilde\chi_2^0)</latex> [GeV] | <latex>m(\tilde\chi_1^\pm)</latex> [GeV] | <latex>m(\tilde\chi_1^0)</latex> [GeV] |  xsec [pb]  |  relative uncertainty  |
|100|80|60|7.61302|0.02396|		
|120|90|60|4.50471|0.02546|		
|81.5|80.75|80|7.74623|0.02308|	
|82|81|80|7.64634|0.02394|
|83|81.5|80|7.45084|0.02409|		
|85|82.5|80|7.07968|0.02417|		
|90|85|80|6.24893|0.02456|
|95|87.5|80|5.53691|0.02499|		
|100|90|80|4.92469|0.02532|		
|110|95|80|3.93372|0.02611|		
|120|100|80|3.18028|0.02680|	
|140|110|80|2.14215|0.02824|	
|101.5|100.75|100|3.20125|0.02627|
|102|101|100|3.16995|0.02694|
|103|101.5|100|3.10963|0.02702|
|105|102.5|100|2.99358|0.02724|
|110|105|100|2.72555|0.02743|
|115|107.5|100|2.48571|0.02791|
|120|110|100|2.27127|0.02814|
|130|115|100|1.90521|0.02896|
|140|120|100|1.60839|0.02944|
|160|130|100|1.16590|0.03099|
|126.5|125.75|125|1.38358|0.02982|
|127|126|125|1.37316|0.03033|
|128|126.5|125|1.35226|0.03053|
|130|127.5|125|1.31280|0.03066|
|135|130|125|1.21990|0.03099|
|140|132.5|125|1.13461|0.03132|
|145|135|125|1.05624|0.03165|
|155|140|125|0.91781|0.03230|
|165|145|125|0.80028|0.03294|
|185|155|125|0.61470|0.03422|
|152|151|150|0.69993|0.03371|
|153|151.5|150|0.69128|0.03370|
|155|152.5|150|0.67448|0.03389|
|160|155|150|0.63450|0.03421|
|165|157.5|150|0.59717|0.03449|
|170|160|150|0.56244|0.03482|
|180|165|150|0.49963|0.03540|
|190|170|150|0.44489|0.03602|
|210|180|150|0.35498|0.03719|
|178|176.5|175|0.39165|0.03627|
|180|177.5|175|0.38342|0.03637|
|185|180|175|0.36371|0.03668|
|190|182.5|175|0.34513|0.03696|
|195|185|175|0.32763|0.03725|
|202|201|200|0.24030|0.03953|
|203|201.5|200|0.23805|0.03953|
|205|202.5|200|0.23362|0.03969|
|210|205|200|0.22295|0.03996|
|215|207.5|200|0.21282|0.04018|
|220|210|200|0.20321|0.04048|
|230|215|200|0.18536|0.04095|
|240|220|200|0.16938|0.04152|
|260|230|200|0.14182|0.04253|
|230|227.5|225|0.15019|0.04177|
|235|230|225|0.14399|0.04203|
|240|232.5|225|0.13808|0.04234|
|252|251|250|0.10281|0.04455|
|253|251.5|250|0.10202|0.04451|
|255|252.5|250|0.10045|0.04469|
|260|255|250|0.09666|0.04492|
|265|257.5|250|0.09296|0.04502|
|270|260|250|0.08954|0.04538|
|280|265|250|0.08293|0.04577|
|290|270|250|0.07698|0.04628|
|310|280|250|0.06636|0.04715|
|302|301|300|0.05032|0.04892|
|303|301.5|300|0.04999|0.04896|
|305|302.5|300|0.04933|0.04904|
|310|305|300|0.04772|0.04925|
|315|307.5|300|0.04611|0.04932|
|320|310|300|0.04467|0.04965|
%ENDTWISTY%

---+++ !C1pC1m (<latex>\tilde\chi_1^+ \tilde\chi_1^-</latex>) Higgsino production 
%TWISTY{mode="div" showlink="Show table " hidelink="Hide table " firststart="hide" showimgright="%ICONURLPATH{toggleopen-small}%" hideimgright="%ICONURLPATH{toggleclose-small}%" remember="on"}%
|  <latex>m(\tilde\chi_2^0)</latex> [GeV] | <latex>m(\tilde\chi_1^\pm)</latex> [GeV] | <latex>m(\tilde\chi_1^0)</latex> [GeV] |  xsec [pb]  |  relative uncertainty  |
|100|80|60|6.66416|0.02753|		
|120|90|60|4.33863|0.02894|		
|81.5|80.75|80|6.45989|0.02651|	
|82|81|80|6.36642|0.02766|
|83|81.5|80|6.22325|0.02773|		
|85|82.5|80|5.95066|0.02788|		
|90|85|80|5.33559|0.02823|
|95|87.5|80|4.80263|0.02859|		
|100|90|80|4.33874|0.02894|		
|110|95|80|3.57416|0.02963|		
|120|100|80|2.97766|0.03031|	
|140|110|80|2.12956|0.03164|	
|101.5|100.75|100|2.90885|0.02975|
|102|101|100|2.87461|0.03045|
|103|101.5|100|2.82433|0.03051|
|105|102.5|100|2.73447|0.03065|
|110|105|100|2.51066|0.03098|
|115|107.5|100|2.30973|0.03131|
|120|110|100|2.12956|0.03164|
|130|115|100|1.81974|0.03229|
|140|120|100|1.56587|0.03288|
|160|130|100|1.17988|0.03417|
|126.5|125.75|125|1.32785|0.03289|
|127|126|125|1.31864|0.03365|
|128|126.5|125|1.29653|0.03374|
|130|127.5|125|1.26094|0.03386|
|135|130|125|1.17722|0.03417|
|140|132.5|125|1.10282|0.03447|
|145|135|125|1.03212|0.03478|
|155|140|125|0.90717|0.03537|
|165|145|125|0.80077|0.03596|
|185|155|125|0.63158|0.03714|
|152|151|150|0.69316|0.03666|
|153|151.5|150|0.68496|0.03675|
|155|152.5|150|0.66905|0.03683|
|160|155|150|0.63127|0.03711|
|165|157.5|150|0.59608|0.03739|
|170|160|150|0.56342|0.03767|
|180|165|150|0.50442|0.03822|
|190|170|150|0.45304|0.03877|
|210|180|150|0.36841|0.03983|
|178|176.5|175|0.39597|0.03885|
|180|177.5|175|0.38795|0.03895|
|185|180|175|0.36877|0.03923|
|190|182.5|175|0.35075|0.03948|
|195|185|175|0.33382|0.03974|
|202|201|200|0.24621|0.04195|
|203|201.5|200|0.24396|0.04201|
|205|202.5|200|0.23956|0.04210|
|210|205|200|0.22897|0.04234|
|215|207.5|200|0.21894|0.04258|
|220|210|200|0.20947|0.04282|
|230|215|200|0.19203|0.04329|
|240|220|200|0.17625|0.04376|
|260|230|200|0.14927|0.04467|
|230|227.5|225|0.15567|0.04387|
|235|230|225|0.14943|0.04409|
|240|232.5|225|0.14348|0.04435|
|252|251|250|0.10732|0.04651|
|253|251.5|250|0.10651|0.04650|
|255|252.5|250|0.10492|0.04663|
|260|255|250|0.10105|0.04684|
|265|257.5|250|0.09736|0.04701|
|270|260|250|0.09383|0.04726|
|280|265|250|0.08722|0.04765|
|290|270|250|0.08117|0.04808|
|310|280|250|0.07052|0.04888|
|302|301|300|0.05317|0.05050|
|303|301.5|300|0.05282|0.05054|
|305|302.5|300|0.05213|0.05061|
|310|305|300|0.05047|0.05080|
|315|307.5|300|0.04886|0.05104|
|320|310|300|0.04733|0.05117|
%ENDTWISTY%

---+++ Branching ratios for <latex>\tilde\chi_2^0 \to \ell \ell \tilde\chi_1^0</latex> and <latex>\tilde\chi_1^\pm \to \ell \nu \tilde\chi_1^0</latex>
%TWISTY{mode="div" showlink="Show table " hidelink="Hide table " firststart="hide" showimgright="%ICONURLPATH{toggleopen-small}%" hideimgright="%ICONURLPATH{toggleclose-small}%" remember="on"}%
| <latex>\Delta M(\tilde\chi_2^0, \tilde\chi_1^0)</latex> [GeV] | <latex>BR(\tilde\chi_2^0 \to ee \tilde\chi_1^0)</latex> | <latex>BR(\tilde\chi_2^0 \to \mu\mu \tilde\chi_1^0)</latex> | <latex>BR(\tilde\chi_2^0 \to \tau\tau \tilde\chi_1^0)</latex> | <latex>BR(\tilde\chi_2^0 \to \ell\ell \tilde\chi_1^0)</latex> | <latex>BR(\tilde\chi_1^\pm \to e \nu \tilde\chi_1^0)</latex> | <latex>BR(\tilde\chi_1^\pm \to \mu \nu \tilde\chi_1^0)</latex> | <latex>BR(\tilde\chi_1^\pm \to \tau \nu \tilde\chi_1^0)</latex> | <latex>BR(\tilde\chi_1^\pm \to \ell \nu \tilde\chi_1^0)</latex> |
|1.0	|0.05292	|0.04979	|0.00000	|0.10271	|0.20804	|0.16782	|0.00000	|0.37586|
|1.5	|0.05112	|0.04981	|0.00000	|0.10093	|0.20375	|0.18498	|0.00000	|0.38873|
|2.0	|0.05087	|0.04881	|0.00000	|0.09968	|0.20220	|0.19140	|0.00000	|0.39360|
|3.0	|0.05016	|0.04924	|0.00000	|0.09940	|0.20100	|0.19610	|0.00000	|0.39710|
|5.0	|0.04714	|0.04681	|0.00471	|0.09866	|0.17790	|0.17630	|0.01053	|0.36473|
|10.0	|0.04285	|0.04279	|0.02670	|0.11235	|0.13180	|0.13150	|0.07201	|0.33531|
|20.0	|0.03801	|0.03800	|0.03385	|0.10985	|0.11660	|0.11650	|0.10000	|0.33310|
|40.0	|0.03537	|0.03537	|0.03482	|0.10556	|0.11253	|0.11251	|0.10817	|0.33321|
|60.0	|0.03498	|0.03498	|0.03458	|0.10454	|0.11170	|0.11170	|0.10980	|0.33320|
%ENDTWISTY%


Main.AlexanderMann - 2019-03-07
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Topic attachments
I	Attachment	History	Action	Size	Date	Who	Comment
in	higgsino_slha.in	r1	manage	47.4 K	2019-03-14 - 18:12	MichaelHelmutHolzbock	templates for slha files
in	higgsino_slha_C1C1.in	r1	manage	47.4 K	2019-03-14 - 18:12	MichaelHelmutHolzbock	templates for slha files
This topic: LHCPhysics > WebHome > SUSYCrossSections > SUSYCrossSections13TeVhinosplit
Topic revision: r7 - 2020-02-04 - AlexanderMann
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