5 research outputs found
Comparative evaluation of analogue front-end designs for the CMS Inner Tracker at the High Luminosity LHC
- Author
- Abbaneo D.
- Abbas M.
- Acosta J. G.
- Adam W.
- Agram J.-L.
- Ahmed I.
- Albergo S.
- Albert A.
- Albert E.
- Alexander J.
- Alhusseini M.
- Allard Y.
- Almeida J.
- Amram O.
- Anagnostou G.
- Andrea J.
- Androsov K.
- Anguiano J.
- Apparu D.
- Ardila L.
- Asenov P.
- Asilar E.
- Assiouras P.
- Azzi P.
- Azzurri P.
- Bacchetta N.
- Backhaus M.
- Bagliesi G.
- Bainbridge R.
- Bakshi A.
- Baldinelli G.
- Balzer M.
- Balázs T.
- Barbagli G.
- Barinoff M.
- Bartek R.
- Bartz E.
- Barvich T.
- Basti A.
- Batista Lopes J.
- Baulieu G.
- Bean A.
- Beaumont W.
- Beccherle R.
- Becerril Gonzalez H.
- Becker R.
- Beghin D.
- Bellan R.
- Benecke A.
- Benelli G.
- Bergamin G.
- Bergauer T.
- Berger P.
- Berry D. R.
- Bertacchi V.
- Bertl W.
- Bethani A.
- Bhardwaj A.
- Bhattacharya R.
- Bianchi F.
- Bianchini L.
- Bilei G. M.
- Bilin B.
- Bisello D.
- Biskop H.
- Bizzaglia S.
- Blanchot G.
- Blank T.
- Blekman F.
- Bloch D.
- Bloom K.
- Blöch D.
- Boccali T.
- Bonnin C.
- Bordlemay Padilla Y.
- Borg J.
- Bortignon P.
- Bosi F.
- Boudoul G.
- Bourgatte G.
- Boyer F.
- Brianzi M.
- Bright-Thonney S.
- Brigljevic V.
- Brivio F.
- Brom J.-M.
- Brown C.
- Bruno G.
- Brzhechko D.
- Brücken E.
- Buhmann P.
- Burkett K.
- Burkle B.
- Bury F.
- Butler D.
- Butz E.
- Bösiger K.
- Calandri A.
- Caminada L.
- Canelli F.
- Canepa A.
- Cannaert E.
- Caponetto L.
- Caprai M.
- Caputo C.
- Caratelli A.
- Cardwell B.
- Cariola P.
- Carnesecchi R.
- Caselle M.
- Cassese A.
- Castaldi R.
- Ceccarelli R.
- Ceresa D.
- Chabert E.
- Chang P.
- Chanon N.
- Charles L.
- Chawla R.
- Checcucci B.
- Chen P.-H.
- Chen X.
- Cheng C.
- Cheng T.
- Cheng Y.
- Chertok M.
- Christiansen J.
- Ciangottini D.
- Ciaranfi R.
- Cichy K.
- Ciocci M. A.
- Ciulli V.
- Civinini C.
- Claes D. R.
- Clement E.
- Clerbaux B.
- Coldham K.
- Cole J.
- Coli S.
- Collard C.
- Connor P.
- Contardo D.
- Conway J.
- Conway J.
- Cooperstein S. B.
- Cormier K.
- Costa M.
- Costa S.
- Coubez X.
- Coughlan J. A.
- Covarelli R.
- Cranshaw D.
- Creanza D.
- Cremaldi L. M.
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- Dangelser E.
- Darej D.
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- Weddigen A.
- Wei K.
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- Zou R.
- Zuber A.
- Zuolo D.
- Šuša T.
- Publication venue
- Institute of Physics Publishing Ltd
- Publication date
- 26/01/2022
- Field of study
Get PDFThe CMS Inner Tracker, made of silicon pixel modules, will be entirely replaced prior to the start of the High Luminosity LHC period. One of the crucial components of the new Inner Tracker system is the readout chip, being developed by the RD53 Collaboration, and in particular its analogue front-end, which receives the signal from the sensor and digitizes it. Three different analogue front-ends (Synchronous, Linear, and Differential) were designed and implemented in the RD53A demonstrator chip. A dedicated evaluation program was carried out to select the most suitable design to build a radiation tolerant pixel detector able to sustain high particle rates with high efficiency and a small fraction of spurious pixel hits. The test results showed that all three analogue front-ends presented strong points, but also limitations. The Differential front-end demonstrated very low noise, but the threshold tuning became problematic after irradiation. Moreover, a saturation in the preamplifier feedback loop affected the return of the signal to baseline and thus increased the dead time. The Synchronous front-end showed very good timing performance, but also higher noise. For the Linear front-end all of the parameters were within specification, although this design had the largest time walk. This limitation was addressed and mitigated in an improved design. The analysis of the advantages and disadvantages of the three front-ends in the context of the CMS Inner Tracker operation requirements led to the selection of the improved design Linear front-end for integration in the final CMS readout chip
Recommended from our members
Comparative evaluation of analogue front-end designs for the CMS Inner Tracker at the High Luminosity LHC
- Author
- Adam W
- Agram JL
- Allard Y
- Andrea J
- Apparu D
- Asilar E
- Beaumont W
- Beghin D
- Bergauer T
- Bethani A
- Bilin B
- Blekman F
- Bloch D
- Blöch D
- Bonnin C
- Bourgatte G
- Brigljevic V
- Brom JM
- Bruno G
- Brücken E
- Bury F
- Caputo C
- Chabert E
- Charles L
- Clerbaux B
- Coldham K
- Cole JE
- Collard C
- D'Hondt J
- Dangelser E
- Darej D
- David P
- De Lentdecker G
- Deblaere A
- Delaere C
- Delcourt M
- Deng W
- Di Croce D
- Donertas IS
- Dragicevic M
- Eerola P
- Favart L
- Ferencek D
- Frühwirth R
- Ghorbani M
- Giammanco A
- Goerlach U
- Grebenyuk A
- Grimault C
- Gross L
- Haas C
- Hinger V
- Hohov D
- Janssen X
- Kalsi A
- Kello T
- Khalilzadeh A
- Khan A
- Krauth M
- Kyberd P
- Lampén T
- Lelek A
- Lemaitre V
- Lowette S
- Luukka P
- Mahdavikhorrami M
- Majumder D
- Makarenko I
- Martikainen L
- Mishra S
- Mondal K
- Moortgat S
- Morton A
- Moureaux L
- Muller D
- Nibigira E
- Ollivier-Henry N
- Popov A
- Postiau N
- Prisciandaro J
- Reid ID
- Robert F
- Roguljic M
- S rensen Bols E
- Sahasransu AR
- Silva Jiménez E
- Song Z
- Starodumov A
- Steininger H
- Szilasi N
- Taliercio A
- Teklishyn M
- Thomas L
- Tuominen E
- Tuuva T
- Van Mechelen P
- Van Putte S
- Van Remortel N
- Vanlaer P
- Vannerom D
- Vischia P
- Wang H
- Wang Q
- Wertz S
- Yang Y
- Šuša T
- Publication venue
- 'IOP Publishing'
- Publication date
- 13/12/2021
- Field of study
Get PDFarXiv preprint available at: https://arxiv.org/abs/2105.00070.Copyright © 2021 CERN for the benefit of the CMS collaboration. The CMS Inner Tracker, made of silicon pixel modules, will be entirely replaced prior to the start of the High Luminosity LHC period. One of the crucial components of the new Inner Tracker system is the readout chip, being developed by the RD53 Collaboration, and in particular its analogue front-end, which receives the signal from the sensor and digitizes it. Three different analogue front-ends (Synchronous, Linear, and Differential) were designed and implemented in the RD53A demonstrator chip. A dedicated evaluation program was carried out to select the most suitable design to build a radiation tolerant pixel detector able to sustain high particle rates with high efficiency and a small fraction of spurious pixel hits. The test results showed that all three analogue front-ends presented strong points, but also limitations. The Differential front-end demonstrated very low noise, but the threshold tuning became problematic after irradiation. Moreover, a saturation in the preamplifier feedback loop affected the return of the signal to baseline and thus increased the dead time. The Synchronous front-end showed very good timing performance, but also higher noise. For the Linear front-end all of the parameters were within specification, although this design had the largest time walk. This limitation was addressed and mitigated in an improved design. The analysis of the advantages and disadvantages of the three front-ends in the context of the CMS Inner Tracker operation requirements led to the selection of the improved design Linear front-end for integration in the final CMS readout chip.The tracker groups gratefully acknowledge financial support from the following funding agencies: BMWFW and FWF (Austria); FNRS and FWO (Belgium); CERN; MSE and CSF (Croatia); Academy of Finland, MEC, and HIP (Finland); CEA and CNRS/IN2P3 (France); BMBF, DFG, and HGF (Germany); GSRT (Greece); NKFIA K124850, and Bolyai Fellowship of the Hungarian Academy of Sciences (Hungary); DAE and DST (India); IPM (Iran); INFN (Italy); PAEC (Pakistan); SEIDI, CPAN, PCTI and FEDER (Spain); Swiss Funding Agencies (Switzerland); MST (Taipei); STFC (United Kingdom); DOE and NSF (U.S.A.). Individuals have received support from HFRI (Greece)
Comparative evaluation of analogue front-end designs for the CMS Inner Tracker at the High Luminosity LHC
- Author
- Abbaneo D.
- Abbas M.
- Acosta J. G.
- Adam W.
- Agram J. -L.
- Ahmed I.
- Albergo S.
- Albert A.
- Albert E.
- Alexander J.
- Alhusseini M.
- Allard Y.
- Almeida J.
- Amram O.
- Anagnostou G.
- Andrea J.
- Androsov K.
- Anguiano J.
- Apparu D.
- Ardila L.
- Asenov P.
- Asilar E.
- Assiouras P.
- Azzi P.
- Azzurri P.
- Bacchetta N.
- Backhaus M.
- Bagliesi G.
- Bainbridge R.
- Bakshi A.
- Balazs T.
- Baldinelli G.
- Balzer M.
- Barbagli G.
- Barinoff M.
- Bartek R.
- Bartz E.
- Barvich T.
- Basti A.
- Batista Lopes J.
- Baulieu G.
- Bean A.
- Beaumont W.
- Beccherle R.
- Becerril Gonzalez H.
- Becker R.
- Beghin D.
- Bellan R.
- Benecke A.
- Benelli G.
- Bergamin G.
- Bergauer T.
- Berger P.
- Berry D. R.
- Bertacchi V.
- Bertl W.
- Bethani A.
- Bhardwaj A.
- Bhattacharya R.
- Bianchi F.
- Bianchini L.
- Bilei G. M.
- Bilin B.
- Bisello D.
- Biskop H.
- Bizzaglia S.
- Blanchot G.
- Blank T.
- Blekman F.
- Bloch D.
- Bloch D.
- Bloom K.
- Boccali T.
- Bonnin C.
- Bordlemay Padilla Y.
- Borg J.
- Bortignon P.
- Bosi F.
- Bosiger K.
- Boudoul G.
- Bourgatte G.
- Boyer F.
- Brianzi M.
- Bright-Thonney S.
- Brigljevic V.
- Brivio F.
- Brom J. -M.
- Brown C.
- Brucken E.
- Bruno G.
- Brzhechko D.
- Buhmann P.
- Burkett K.
- Burkle B.
- Bury F.
- Butler D.
- Butz E.
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- Zou R.
- Zuber A.
- Zuolo D.
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2021
- Field of study
No full textThe CMS Inner Tracker, made of silicon pixel modules, will be entirely replaced prior to the start of the High Luminosity LHC period. One of the crucial components of the new Inner Tracker system is the readout chip, being developed by the RD53 Collaboration, and in particular its analogue front-end, which receives the signal from the sensor and digitizes it. Three different analogue front-ends (Synchronous, Linear, and Differential) were designed and implemented in the RD53A demonstrator chip. A dedicated evaluation program was carried out to select the most suitable design to build a radiation tolerant pixel detector able to sustain high particle rates with high efficiency and a small fraction of spurious pixel hits. The test results showed that all three analogue front-ends presented strong points, but also limitations. The Differential front-end demonstrated very low noise, but the threshold tuning became problematic after irradiation. Moreover, a saturation in the preamplifier feedback loop affected the return of the signal to baseline and thus increased the dead time. The Synchronous front-end showed very good timing performance, but also higher noise. For the Linear front-end all of the parameters were within specification, although this design had the largest time walk. This limitation was addressed and mitigated in an improved design. The analysis of the advantages and disadvantages of the three front-ends in the context of the CMS Inner Tracker operation requirements led to the selection of the improved design Linear front-end for integration in the final CMS readout chip
Comparative evaluation of analogue front-end designs for the CMS Inner Tracker at the High Luminosity LHC
- Author
- Abbaneo D.
- Abbas M.
- Acosta J. G.
- Adam W.
- Agram J.-L.
- Ahmed I.
- Albergo S.
- Albert A.
- Albert E.
- Alexander J.
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- Coughlan J. A.
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- Creanza D.
- Cremaldi L. M.
- Cumalat J. P.
- Curras Rivera E.
- Cussans D.
- Daguin J.
- Dangelser E.
- Darej D.
- Das A.
- Das S.
- Daskalakis G.
- Datta A.
- David P.
- De Boer W.
- De Lentdecker G.
- De Palma M.
- De Robertis G.
- De Wit A.
- Deblaere A.
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- Del Burgo R.
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- Demiragli Z.
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- Dickinson J.
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- Djambazov L.
- Dolen J.
- Dominguez A.
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- Donega M.
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- Dorfer C.
- Dorigo T.
- Dragicevic M.
- Droll A.
- Duarte Campderros J.
- Dudek M.
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- Dupasquier T.
- Durgut S.
- Dutta S.
- Dutta V.
- Dziwok C.
- D’Alessandro R.
- D’Angelo P.
- D’Hondt J.
- Ebrahimi A.
- Eckerlin G.
- Ecklund K. M.
- Eckstein D.
- Eerola P.
- Eich M.
- El Morabit K.
- Eminizer N.
- Emriskova N.
- Erdmann W.
- Eusebi R.
- Evdokimov A.
- Evdokimov O.
- Faccio F.
- Fan L.
- Fangmeier C.
- Farnesini L.
- Favart L.
- Fedi G.
- Feindt F.
- Feld L.
- Ferencek D.
- Fernandez M.
- Ferro F.
- Filenius A.
- Fiore L.
- Fiori F.
- Fluegge G.
- Focardi E.
- Ford W. T.
- Francis B.
- Frank N.
- Freed S.
- French T.
- Froehlich A.
- Frühwirth R.
- Gaioni L.
- Galbit G.
- Gallo E.
- Gandrakotra A.
- Garbolino S.
- Garcia Alonso A.
- Garutti E.
- Gastler D.
- Gennai S.
- Gerber C. E.
- Gerosa R.
- Gershtein Y.
- Ghorbani M.
- Ghosh A.
- Giammanco A.
- Giannini L.
- Giassi A.
- Gingu C.
- Glessgen F.
- Goerlach U.
- Goldstein J.
- Golf F.
- Gomez G.
- Gonzalez Sanchez F. J.
- Gonzalez H.
- Gouskos L.
- Grab C.
- Grebenyuk A.
- Grimault C.
- Grippo M.
- Grippo M. T.
- Gritsan A.
- Gross L.
- Grünendahl S.
- Gunnellini P.
- Guthoff M.
- Guzzi L.
- Haas C.
- Hahn K.
- Hajheidari M.
- Halkiadakis E.
- Hall G.
- Haller J.
- Hanson G.
- Harb A.
- Harder K.
- Hart A.
- Hartmann F.
- Haza G.
- Hazen E.
- Heintz U.
- Hemer D.
- Hill C. S.
- Hindrichs O.
- Hinger V.
- Hinton N.
- Hinzmann A.
- Hits D.
- Hofman D. J.
- Hogan J.
- Hogan S.
- Hohov D.
- Hollos A.
- Holmberg M.-L.
- Honma A.
- Horisberger R.
- Horyn L. A.
- Hou W.-S.
- Hugo G.
- Husemann U.
- Huwiler M.
- Iashvili I.
- Incandela J.
- Ince M.
- Ionica M.
- Ivanov A.
- Jabusch H.
- Jain C.
- Jain G.
- Jain S.
- Janssen X.
- Jaramillo Echeverria R.
- Jensen F.
- Jofrehei A.
- Johns W.
- Johnson M.
- Jones M.
- Joo C.
- Jung A.
- Kaestli H.-C.
- Kalsi A.
- Kaplon J.
- Kar C.
- Karpinski W.
- Kasieczka G.
- Kazas I.
- Kello T.
- Kerekes Z.
- Khalil S.
- Khalilzadeh A.
- Khan A.
- Kharchilava A.
- Kilminster B.
- Kilpatrick M.
- Klabbers P.
- Klanner R.
- Klein K.
- Kleinwort C.
- Kloukinas K.
- Koppenhöfer R.
- Korotkov A.
- Koshy A.
- Koss N.
- Kotlinski D.
- Kottelat L.
- Koukola D.
- Kovacs M.
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- Publication venue
- 'IOP Publishing'
- Publication date
- 11/12/2020
- Field of study
Get PDFInternational audienceThe CMS Inner Tracker, made of silicon pixel modules, will be entirely replaced prior to the start of the High Luminosity LHC period. One of the crucial components of the new Inner Tracker system is the readout chip, being developed by the RD53 Collaboration, and in particular its analogue front-end, which receives the signal from the sensor and digitizes it. Three different analogue front-ends (Synchronous, Linear, and Differential) were designed and implemented in the RD53A demonstrator chip. A dedicated evaluation program was carried out to select the most suitable design to build a radiation tolerant pixel detector able to sustain high particle rates with high efficiency and a small fraction of spurious pixel hits. The test results showed that all three analogue front-ends presented strong points, but also limitations. The Differential front-end demonstrated very low noise, but the threshold tuning became problematic after irradiation. Moreover, a saturation in the preamplifier feedback loop affected the return of the signal to baseline and thus increased the dead time. The Synchronous front-end showed very good timing performance, but also higher noise. For the Linear front-end all of the parameters were within specification, although this design had the largest time walk. This limitation was addressed and mitigated in an improved design. The analysis of the advantages and disadvantages of the three front-ends in the context of the CMS Inner Tracker operation requirements led to the selection of the improved design Linear front-end for integration in the final CMS readout chip
Hard color-singlet exchange in dijet events in proton-proton collisions at s= 13 TeV
- Author
- Aarrestad Thea Klaeboe
- Aarup Petersen Henriette
- Abbaneo Duccio
- Abbiendi Giovanni
- Abbrescia Marcello
- Abdelalim Ahmed Ali
- Abdullin Salavat
- Abercrombie Daniel
- Abu Zeid Shimaa
- Acharya Himal
- Acosta Darin
- Acosta John Gabriel
- Adam Wolfgang
- Adams Eric
- Adams Mark Raymond
- Adams Todd
- Adloff Catherine
- Adzic Petar
- Afanasiev Serguei
- Agapitos Antonis
- Agarwal Garvita
- Aggleton Robin
- Agram Jean-Laurent
- Aguilar-Benitez Manuel
- Ahmad Ashfaq
- Ahmad Muhammad
- Ahmed Asar
- Ahuja Sudha
- Akchurin Nural
- Akgun Bora
- Akpinar Alp
- Albajar Carmen
- Albergo Sebastiano
- Albert Andreas
- Albrow Michael
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- Allen Brandon
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- Alvarez Gonzalez Barbara
- Alverson George
- Alves Gilvan
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- Alyari Maral
- Amapane Nicola
- Ambrogi Federico
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- Amram Oz
- Amsler Claude
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- Andrews Michael Benjamin
- Androsov Konstantin
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- He He
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- Heredia-De La Cruz Ivan
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- Ivanchenko Vladimir N
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- Norberg Scarlet
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- Zalewski Piotr
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- Zarucki Mateusz
- Zecchinelli Angelo Giacomo
- Zenaiev Oleksandr
- Zenz Seth Conrad
- Zeuner Wolfram Dietrich
- Zghiche Amina
- Zhang Aobo
- Zhang Fengwangdong
- Zhang Huaqiao
- Zhang Jingyu
- Zhang Sijing
- Zhang Wenyu
- Zhang Yi
- Zhang Zhicai
- Zhao Jingzhou
- Zhokin Alexander
- Zhu De Hua
- Zhu Ren-Yuan
- Zich Jan
- Zielinski Krzysztof Jan
- Ziemons Tim
- Zientek Margaret
- Zlebcik Radek
- Zobec Joze
- Zoi Irene
- Zolkapli Zukhaimira
- Zorbakir Ibrahim Soner
- Zorbilmez Caglar
- Zotto Pierluigi
- Zou David
- Zucchetta Alberto
- Zumerle Gianni
- Zuo Xunwu
- Zuolo Davide
- Zygala Lara
- Álvarez Fernández Adrian
- Österberg Kenneth Mikael
- Özçelik Özlem
- Široký Jan
- Publication venue
- American Physical Society
- Publication date
- 01/01/2021
- Field of study
Get PDFInternational audienceEvents where the two leading jets are separated by a pseudorapidity interval devoid of particle activity, known as jet-gap-jet events, are studied in proton-proton collisions at s= 13 TeV. The signature is expected from hard color-singlet exchange. Each of the highest transverse momentum (pT) jets must have pTjet> 40 GeV and pseudorapidity 1.4 <∣ηjet∣< 4.7, with ηjet1ηjet2< 0, where jet1 and jet2 are the leading and subleading jets in pT, respectively. The analysis is based on data collected by the CMS and TOTEM experiments during a low luminosity, high-β∗ run at the CERN LHC in 2015, with an integrated luminosity of 0.66 pb−1. Events with a low number of charged particles with pT> 0.2 GeV in the interval ∣η∣< 1 between the jets are observed in excess of calculations that assume only color-exchange. The fraction of events produced via color-singlet exchange, fCSE, is measured as a function of pTjet2, the pseudorapidity difference between the two leading jets, and the azimuthal angular separation between the two leading jets. The fraction fCSE has values of 0.4-1.0%. The results are compared with previous measurements and with predictions from perturbative quantum chromodynamics. In addition, the first study of jet-gap-jet events detected in association with an intact proton using a subsample of events with an integrated luminosity of 0.40 pb−1 is presented. The intact protons are detected with the Roman pot detectors of the TOTEM experiment. The fCSE in this sample is 2.91 ± 0.70 (stat) −1.01+1.08 (syst) times larger than that for inclusive dijet production in dijets with similar kinematics
