35 research outputs found
Dental pulp tissue engineering
- Author
- Arana-Chavez VE
- Barnes CP
- Batouli S
- Bjorndal L
- Brey EM
- Bruno Neves Cavalcanti
- Casagrande L
- Chrobak KM
- Cordeiro MM
- d'Aquino R
- Decup F
- Demarco FF
- Demarco FF
- Flávio Fernando Demarco
- Galler KM
- Gandia C
- Goldberg M
- Goldberg M
- Goldberg M
- Gomes JA
- Goncalves SB
- Graziano A
- Gronthos S
- Gronthos S
- Hargreaves KM
- Huang GT
- Huang GT
- Huang GT
- Huang GT
- Iohara K
- Jacques Eduardo Nör
- Jazayeri M
- Jepsen S
- Kerkis
- Kim GD
- Langer R
- Lokmic Z
- Luciano Casagrande
- Marchionni C
- Marcus Cristian Muniz Conde
- Martin I
- Maxwell PH
- Melero-Martin JM
- Misawa H
- Miura M
- Mjor IA
- Morsczeck C
- Morsczeck C
- Mullane EM
- Murphy WL
- Murphy WL
- Muschler GF
- Nakashima M
- Nakashima M
- Nakashima M
- Nakashima M
- Narmoneva
- Nedel F
- Nor JE
- Nor JE
- Nor JE
- Park IH
- Park IH
- Peters MC
- Prockop DJ
- Raff M
- Roberts-Clark DJ
- Rosa V
- Ruch JV
- Rutherford RB
- Sakai VT
- Seo BM
- Shieh SJ
- Six N
- Six N
- Smith AG
- Smith AJ
- Smith AJ
- Sonoyama W
- Sonoyama W
- Stevens MM
- Tamaoki N
- Thesleff I
- Thomson JA
- Thonhoff JR
- Tomson PL
- Tran-Hung L
- Tran-Hung L
- Tziafas D
- Villar CC
- Vivien Thiemy Sakai
- Volponi AA
- Wang J
- Wei G
- Yang S
- Zhang W
- Publication venue
- 'FapUNIFESP (SciELO)'
- Publication date
- 01/01/2011
- Field of study
The use of differential photocalorimetry to measure the oxidation induction time of isotatic polypropylene
- Author
- Publication venue
- Inglaterra
- Publication date
- Field of study
The widespread use of polymeric materials in many applications requires polymers which are weather resistant. The aim of this study is to examine the usefulness of oxidation induction time (OIT) measurements by differential photocalorimetry (DPC) as a tool for evaluating the ultraviolet (UV) stability of isotatic polypropylene (PPi). DPC was used to measure OIT in PPi formulations containing different concentrations of light and thermal stabilizers. The OIT was measured with and without UV light incidence and the results were compared with the appearance of cracks seen with an optical microscopy, after aging in a Weather-Ometer. The measures of OIT with UV light showed values 25-60% smaller than the values of OIT without light, for different formulations. In this paper, these OIT results will be discussed. (C) 2003 Elsevier Ltd. All rights reserved.23446146
Use of oxidation onset temperature measurements for evaluating the oxidative degradation of isotatic polypropylene
- Author
- Publication venue
- EUA
- Publication date
- Field of study
The widespread use of polymeric materials in many applications requires polymers that are weather resistant. The aim of this study is to examine the usefulness of oxidation onset temperature measurements as a tool for evaluating oxidative degradation of isotatic polypropylene. Differential scanning calorimetry was used to measure the oxidation onset temperature in formulations of isotatic polypropylene containing different concentrations of light and thermal stabilizers after aging in a Weather-Ometer. Oxidation onset temperature gave better results than oxidation induction time for evaluating the degradation of isotatic polypropylene during aging in a Weather-Ometer. However, both tests showed a poor correlation with the appearance of cracks seen by optical microscopy.121111
Electroweak parameters of the z0 resonance and the standard model
- Author
- Abbaneo D
- ABREU P
- Adam W
- Adami F
- ADEVA B
- Adriani O
- Adye T
- Aguilar-Benitez M
- Ajaltouni Z
- Akbari H
- Akesson T
- Albanese JP
- Alcaraz J
- Alekseev GD
- Alemany R
- Alexander G
- Allen P
- Allison J
- Allport PP
- Almehed S
- Aloisio A
- Alted F
- Altoon B
- Alverson G
- Alviggi MG
- Alvsvaag SJ
- Amaldi U
- Amendolia SR
- An Q
- Anassontzis EG
- Anderhub H
- Anderson AL
- Anderson KJ
- Andreev VP
- Angelov T
- Antilogus P
- Antonelli A
- Antonov L
- Antreasyan D
- Apel WD
- Apollinari G
- Arce P
- Arcelli S
- Arefev A
- Armitage JC
- Ashman JG
- Ashton P
- Asman B
- Astbury A
- Astier P
- Atwood WB
- Aubert JJ
- Augustin JE
- Augustinus A
- Axen D
- Azemoon T
- Aziz T
- Azuelos G
- Baba PVKS
- Badier J
- Bagliesi G
- Bagnaia P
- Bahan GA
- Baillon P
- Baines JTM
- Bakken JA
- Baksay L
- Baldini R
- Ball AH
- Ball RC
- Bambade P
- Banerjee S
- Banks J
- Bao J
- Barao F
- Barberio E
- Barbiellini G
- Barczewski T
- Bardadin-Otwinowska M
- Bardin DY
- Barker GJ
- Barlow RJ
- Baroncelli A
- Barone L
- Barring O
- Bartl W
- Bates MJ
- Batignani G
- Batley JR
- Battaglia M
- Baubillier M
- Bauerdick LAT
- Bay A
- Beaudoin G
- Beck A
- Becker J
- Becker U
- Becket H
- Becks KH
- Beeston CJ
- Begalli M
- Behnke T
- Behrens J
- Beilliere P
- Beingessner S
- Belk AT
- Bell KW
- Bella G
- Bellantoni L
- Belokopytov YA
- Belokopytov YA
- Beltran P
- Beltran P
- Benchouk C
- Bencivenni G
- Bencze GL
- Benedic D
- Benedic D
- Benlloch JM
- Benlloch JM
- Berdugo J
- Berges P
- Berggren M
- Berggren M
- Bernard V
- Bertin V
- Bertrand D
- Bertrand D
- Bertucci B
- Betev BL
- Betheke S
- Beuselinck R
- Biagi SF
- Biagi SF
- Bianchi F
- Bianchi F
- Bibby JH
- Bibby JH
- Biebel O
- Biland A
- Bilenky SM
- Bilenky SM
- Billoir P
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- Binder U
- Binnie DM
- Bird F
- Bizzarri R
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- Blaising JJ
- Bloch D
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- Bloemeke P
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- Chang CY
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- Charlton DG
- Charpentier P
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- Chelkov GA
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- Djama F
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- Duckeck G
- Duerdoth IP
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- Duinker P
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- Duran I
- Dydak F
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- Eckerlin G
- Edgecock TR
- Edwards M
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- Eerola PAM
- Efthymiopoulos I
- Ekelof TJC
- Ekspong G
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- Eppling FJ
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- Yin ZW
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- Yzerman M
- Zaccardelli C
- Zacharov I
- Zaitsev A
- Zalewska-Bak A
- Zalewski P
- Zehnder L
- Zemp P
- Zeng M
- Zeng Y
- Zeuner W
- Zevgolatakos E
- Zhang DH
- Zhang G
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- Zichichi A
- Zimin NI
- Zito G
- Zito M
- Zitoun R
- Zobernig G
- Zografou P
- Zomer F
- Zorn GT
- Zukanovich-Funchal R
- Zumerle G
- Zuniga J
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/1992
- Field of study
Contains fulltext :
124399.pdf (publisher's version ) (Open Access
Cryopreservation Effects on Wharton’s Jelly Stem Cells Proteome
- Author
- A Bheda
- A Bongso
- A Castegna
- A Maruko
- A. Riviello
- AA Volponi
- AX Liu
- BC Heng
- BC Heng
- C Csaki
- C Gandia
- C Holden
- C Tomasetto
- C. Di Ilio
- CJ Hunt
- CM Kashuba Benson
- CM Pickart
- CR Sihn
- CY Fong
- CY Fong
- D Gao
- DW Kim
- DW Owens
- E Erba
- E Rieser
- E Tzima
- E. Eleuterio
- F Boer de
- F Foertsch
- F Shang
- F. Di Giuseppe
- G Chamberlain
- G Krzysiek-Maczka
- G Wettsteina
- G. Bologna
- GL Blatch
- GR Buettner
- H Johansoson
- HS Wang
- I Zemp
- J Tucholski
- JE Carroll
- JG Baust
- JY Hsieh
- K Gauthaman
- K Gauthaman
- K Lima Prata de
- K Nakamura
- L Fésüs
- L Fésüs
- L. Pierdomenico
- M Chevallet
- M Ni
- M Perluigi
- M. Gesi
- M. Marchisio
- M. Sulpizio
- MA Antonyak
- MA Mackinder
- MF Olson
- MH Glickman
- P Lanuti
- P Lanuti
- P. Lanuti
- PR Sanberg
- PS Mathieu
- R Moll
- S Angelucci
- S Fourquet
- S Jomura
- S Miscia
- S Thirumala
- S. Angelucci
- S. Miscia
- SO Lim
- SP Perfetto
- T Bakhshi
- T Rabilloud
- TG Grunewald
- TN Hansen
- V Bizzarro
- V Gatta
- X Xu
- X Xu
- Y Kaneko
- Y Liu
- YA Romanov
- Z Miao
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
The reaction e+ e- ---> gamma gamma (gamma) at Z0 energies
- Author
- ABREU P
- ADAM W
- ADAMI F
- ADYE T
- AGUERA MAL
- AKESSON T
- ALEKSEEV GD
- ALLEN P
- ALMEHED S
- ALONSO MF
- ALTED F
- ALVSVAAG SJ
- AMALDI U
- ANASSONTZIS E
- ANTILOGUS P
- APEL WD
- APSIMON RJ
- ASMAN B
- ASTIER P
- AUGUSTIN JE
- AUGUSTINUS A
- BAILLON P
- BAMBADE P
- BARAO F
- BARBIELLINI G
- BARDIN DY
- BARONCELLI A
- BARRING O
- BARTL W
- BATES MJ
- BATTAGLIA M
- BAUBILLIER M
- BECKS KH
- BEESTON CJ
- BEGALLI M
- BEILLIERE P
- BELOKOPYTOV Y
- BELTRAN P
- BENEDIC D
- BENLLOCH JM
- BERGGREN M
- BERTRAND D
- BIAGI S
- BIANCHI F
- BIBBY JH
- BILENKY MS
- BILLOIR P
- BJARNE J
- BLOCH D
- BLYTH S
- BOGOLUBOV PN
- BOLOGNESE T
- BONAPART M
- BONESINI M
- BONIVENTO W
- BOOTH PSL
- BORATAV M
- BORGEAUD P
- BORISOV G
- BORNER H
- BOSIO C
- BOTNER O
- BOUQUET B
- BOZZO M
- BRAIBANT S
- BRANCHINI P
- BRAND KD
- BRENNER RA
- BRICMAN C
- BROWN RCA
- BRUMMER N
- BRUNET JM
- BUGGE L
- BURAN T
- BURMEISTER H
- BUYTAERT JAMA
- CACCIA M
- CADENAS JJGY
- CALVI M
- CAMPAGNE JE
- CAMPION A
- CAMPORESI T
- CANALE V
- CAO F
- CARROLL L
- CASO C
- CASTELLI E
- CATTAI A
- CAVALLO FR
- CERRITO L
- CHARPENTIER P
- CHECCHIA P
- CHELKOV GA
- CHEVALIER L
- CHLIAPNIKOV P
- CHOROWICZ V
- CIRIO R
- CLARA MP
- COLLINS P
- CONTRERAS JL
- CONTRI R
- COSME G
- COUCHOT F
- CRAWLEY HB
- CRENNELL D
- CROSETTI G
- CROSLAND N
- CROZON M
- CZELLAR S
- DAGORET S
- DAHLJENSEN E
- DALMAGNE B
- DAM M
- DAMGAARD G
- DARBO G
- DAUBIE E
- DAUNCEY PD
- DAVENPORT M
- DAVID P
- DEANGELIS A
- DEBEER M
- DEBOECK H
- DEBOER W
- DECLERCQ C
- DEFOIX C
- DEGROOT N
- DELAVAISSIERE C
- DELIKARIS D
- DELORME S
- DELOTTO B
- DELPIERRE P
- DEMARIA N
- DEMIN A
- DEMONCHENAULT GH
- DERKAOUI J
- DICIACCIO L
- DIJKSTRA H
- DJAMA F
- DOLBEAU J
- DONSZELMANN M
- DOROBA K
- DRACOS M
- DREES J
- DRIS M
- DUFOUR Y
- DULINSKI W
- DZHELYADIN R
- EEK LO
- EEROLA PAM
- EKELOF T
- EKSPONG G
- ENGEL JP
- FASSOULIOTIS D
- FENYUK A
- FERRER A
- FERRER JAV
- FILIPPAS TA
- FIRESTONE A
- FOETH H
- FOKITIS E
- FOLEGATI P
- FONTANELLI F
- FORSBACH H
- FRANEK B
- FRENKIEL P
- FRIES DC
- FRODESEN AG
- FRUHWIRTH R
- FULDAQUENZER F
- FUNCHAL RZ
- FURNIVAL K
- FURSTENAU H
- FUSTER J
- GAGO JM
- GALEAZZI G
- GAMBA D
- GARCIA C
- GARCIA J
- GASPARINI U
- GAVILLET P
- GAZIS EN
- GERBER JP
- GIACOMELLI P
- GIMENEZ MVC
- GLITZA KW
- GOKIELI R
- GOLOVATYUK VM
- GOOBAR A
- GOPAL G
- GORSKI M
- GRACCO V
- GRANT A
- GRARD F
- GRAZIANI E
- GROS MH
- GROSDIDIER G
- GROSSETETE B
- GUMENYUK S
- GUY J
- HAHN F
- HAHN M
- HAIDER S
- HAJDUK Z
- HAKANSSON A
- HALLGREN A
- HAMACHER K
- HARRIS FJ
- HECK BW
- HERBST I
- HERNANDEZ JJ
- HERQUET P
- HERR H
- HIETANEN I
- HIGON E
- HILKE HJ
- HODGSON SD
- HOFMOKL T
- HOLMES R
- HOLMGREN SO
- HOLTHUIZEN D
- HONORE PF
- HOOPER JE
- HOULDEN M
- HRUBEC J
- HULTH PO
- HULTQVIST K
- HUSSON D
- HYAMS BD
- IOANNOU P
- ISENHOWER D
- IVERSEN PS
- JACKSON JN
- JALOCHA P
- JARLSKOG G
- JARRY P
- JEANMARIE B
- JOHANSSON EK
- JOHNSON D
- JONKER M
- JONSSON L
- JUILLOT P
- KALKANIS G
- KALMUS G
- KANTARDJIAN G
- KAPUSTA F
- KATARGIN A
- KATSANEVAS S
- KATSOUFIS EC
- KERANEN R
- KESTEMAN J
- KHOMENKO BA
- KHOVANSKI NN
- KING B
- KJAER NJ
- KLEIN H
- KLEMPT W
- KLOVNING A
- KLUIT P
- KOEHNE JH
- KOENE B
- KOKKINIAS P
- KOPF M
- KORATZINOS M
- KORCYL K
- KORYTOV AV
- KORZEN B
- KOSTUKHIN V
- KOURKOUMELIS C
- KREUZBERGER T
- KROLIKOWSKI J
- KRUENERMARQUIS U
- KRUPINSKI W
- KUCEWICZ W
- KURVINEN K
- LACASTA C
- LAMBROPOULOS C
- LAMSA JW
- LANCERI L
- LAPIN V
- LASO MDMD
- LAUGIER JP
- LAUHAKANGAS R
- LEDER G
- LEDROIT F
- LEMONNE J
- LENZEN G
- LEPELTIER V
- LETESSIERSELVON A
- LIEB E
- LIKO D
- LILLETHUN E
- LINDGREN J
- LIPNIACKA A
- LIPPI I
- LLOSA R
- LOERSTAD B
- LOKAJICEK M
- LOKEN JG
- LOPEZFERNANDEZ A
- LOS M
- LOUKAS D
- LOUNIS A
- LOZANO JJ
- LUCOCK R
- LUTZ P
- LYONS L
- MAEHLUM G
- MAESTRO JC
- MAILLARD J
- MALTEZOS A
- MALTEZOS S
- MANDL F
- MARCO J
- MARGONI M
- MARIN JC
- MARKOU A
- MARTI S
- MATHIS L
- MATORRAS F
- MATTEUZZI C
- MATTHIAE G
- MAZZUCATO M
- MCCUBBIN M
- MCKAY R
- MCNULTY R
- MENICHETTI E
- MERONI C
- MEYER WT
- MICHELOTTO M
- MITAROFF WA
- MITSELMAKHER GV
- MJOERNMARK U
- MOA T
- MOELLER R
- MOENIG K
- MONGE MR
- MORETTINI P
- MUELLER H
- MULLER H
- MURRAY WJ
- MYATT G
- NARAGHI F
- NAUKORZEN U
- NAVARRIA FL
- NEGRI P
- NIELSEN BS
- NIJJHAR B
- NIKOLAENKO V
- OBRAZTSOV V
- OLSHEVSKI AG
- ORAVA R
- OSTANKOV A
- OURAOU A
- PAIN R
- PALKA H
- PAPADOPOULOU T
- PAPE L
- PASSERI A
- PEGORARO M
- PEISERT AE
- PEREVOZCHIKOV V
- PERNICKA M
- PERROTTA A
- PIERRE F
- PIMENTA M
- PINGOT O
- PINSENT A
- POL ME
- POLOK G
- POROPAT P
- PRIVITERA P
- PULLIA A
- PYYHTIA J
- RADOJICIC D
- RAGAZZI S
- RANGE WH
- RATOFF PN
- READ AL
- REDAELLI NG
- REGLER M
- REID D
- RENTON PB
- RESVANIS LK
- RICHARD F
- RICHARDSON M
- RIDKY J
- RINAUDO G
- RODITI I
- ROMERO A
- RONCAGLIOLO I
- RONCHESE P
- RONNQVIST C
- ROSENBERG EI
- ROSSI U
- ROSSO E
- ROUDEAU P
- ROVELLI T
- ROZAS AJC
- RUCKSTUHL W
- RUHLMANN V
- RUIZ A
- RYBICKI K
- SAARIKKO H
- SACQUIN Y
- SALT J
- SANCHEZ E
- SANCHEZ J
- SANNINO M
- SCHAEFFER M
- SCHAEL S
- SCHNEIDER H
- SCURI F
- SEGAR AM
- SEKULIN R
- SESSA M
- SETTE G
- SEUFERT R
- SHELLARD RC
- SIEGRIST P
- SIMONETTI S
- SIMONETTO F
- SISSAKIAN AN
- SKAALI TB
- SKJEVLING G
- SMADJA G
- SMITH GR
- SOSNOWSKI R
- SPASSOFF TS
- SPIRITI E
- SQUARCIA S
- STAECK H
- STANESCU C
- STAVROPOULOS G
- STICHELBAUT F
- STOCCHI A
- STRAUSS J
- STRUB R
- STUBENRAUCH CJ
- SZCZEKOWSKI M
- SZEPTYCKA M
- SZYMANSKI P
- TABARELLI T
- TAVERNIER S
- THEODOSIOU GE
- TILQUIN A
- TIMMERMANS J
- TIMOFEEV VG
- TKATCHEV LG
- TODOROV T
- TOET DZ
- TORTORA L
- TRAINOR MT
- TREILLE D
- TREVISAN U
- TRISCHUK W
- TRISTRAM G
- TRONCON C
- TSIROU A
- TSYGANOV EN
- TURALA M
- TURCHETTA R
- TURLUER ML
- TUUVA T
- TYAPKIN IA
- TYNDEL M
- TZAMARIAS S
- UEBERSCHAER B
- UEBERSCHAER S
- ULLALAND O
- UVAROV VA
- VALENTI G
- VALLAZZA E
- VANAPELDOORN GW
- VANDAM P
- VANDERVELDE C
- VANDONINCK WK
- VANEIJNDHOVEN N
- VARELA J
- VAZ P
- VEGNI G
- VELASCO J
- VENTURA L
- VENUS W
- VERBEURE F
- VERTOGRADOV LS
- VIBERT L
- VILANOVA D
- VLASOV EV
- VODOPYANOV AS
- VOLLMER M
- VOLPONI S
- VOULGARIS G
- VOUTILAINEN M
- VRBA V
- WAHLEN H
- WALCK C
- WALDNER F
- WAYNE M
- WEILHAMMER P
- WERNER J
- WETHERELL AM
- WICKENS JH
- WIKNE J
- WILKINSON GR
- WILLIAMS WSC
- WINTER M
- WORMALD D
- WORMSER G
- WOSCHNAGG K
- YAMDAGNI N
- YEPES P
- ZAITSEV A
- ZALEWSKA A
- ZALEWSKI P
- ZEVGOLATAKOS E
- ZHANG G
- ZIMIN NI
- ZITO M
- ZITOUN R
- ZUMERLE G
- ZUNIGA J
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/1991
- Field of study
The total and differential cross-sections for the reaction e+e- → γγ(γ) are measured at centre of mass energies around 91 GeV using an integrated luminosity of 4.7 pb-1. The aggreement with QED prediction is good. Consequently there is no evidence for non-standard channels which would have the same experimental signature. The lower limits on the QED cuttoff parameters are Λ+ > 113 GeV and Λ- > 95 GeV. An upper limit on the effective coupling between a possible excited electron and the gamma is derived. At 95% confidence level the branching ratios for Z0 decay into π0γ, ηψ and γγγ are below 1.5 × 10-4, 2.8 × 10-4 and 1.4 × 10-4 respectively.0info:eu-repo/semantics/publishe
STUDY OF ORIENTATION OF 3-JET EVENTS IN Z(0) HADRONIC DECAYS USING THE DELPHI DETECTOR
- Publication venue
- Publication date
- 01/01/1992
- Field of study
The study of the orientation of three-jet events from e+ e- –> Z0 –>
multi-hadrons is presented, in particular the polar angle distributions
of the thrust axis and of the normal to the three-jet plane, and the
azimuthal correlations between the hadron plane and the one defined by
the beam and thrust axes. The data are compared with results at lower
energy and with QCD predictions. Good agreement with QCD predictions is
observed. The scalar gluon theory is excluded by the data
A MEASUREMENT OF THE LIFETIME OF THE TAU-LEPTON
- Publication venue
- Publication date
- 01/01/1991
- Field of study
The lifetime of the tau lepton has been measured by two independent
methods using a silicon microvertex detector installed in the DELPHI
detector. The signed impact parameter distribution of the one prong
decays yielded a lifetime of tau-tau = 321 +/- 36 (stat.) +/- 16 (syst.)
fs, while the decay length distribution of three prong decays gave the
result tau-tau = 310 +/- 31 (stat. ) +/- 9 (syst.) fs. The final value
of the combined result was tau-tau = 314 +/- 25 fs. The ratio of the
Fermi coupling constant from tau decay relative to that from muon decay
was found to be 0.95 +/- 0.04, compatible with the hypothesis of lepton
universality
THE REACTION E+E--] GAMMA-GAMMA(GAMMA) AT Z0 ENERGIES
- Publication venue
- Publication date
- 01/01/1991
- Field of study
The total and differential cross-sections for the reaction e+e- –>
gamma-gamma(gamma) are measured at centre of mass energies around 91 GeV
using an integrated luminosity of 4.7 pb-1. The agreement with the QED
prediction is good. Consequently there is no evidence for non-standard
channels which would have the same experimental signature. The lower
limits on the QED cutoff parameters are LAMBDA+ > 113 GeV and LAMBDA- >
95 GeV. An upper limit on the effective coupling between a possible
excited electron and the gamma is derived. At 95% confidence level the
branching ratios for Z0 decay into pi-0-gamma, eta-gamma and
gamma-gamma-gamma are below 1.5 x 10(-4), 2.8 x 10(-4) and 1.4 x 10(-4)
respectively
DETERMINATION OF Z0 RESONANCE PARAMETERS AND COUPLINGS FROM ITS HADRONIC AND LEPTONIC DECAYS
- Publication venue
- Publication date
- 01/01/1991
- Field of study
From measurements of the cross sections for e+ e - –> hadrons and the
cross sections and forward-backward charge-asymmetries for e+ e- –> e+
e-, mu+ mu- and tau+ tau- at several centre-of-mass energies around the
Z0 pole with the DELPHI apparatus, using approximately 150000 hadronic
and leptonic events from 1989 and 1990, one determines the following Z0
parameters: the mass and total width M(Z) = 91.177 +/- 0.022 GeV,
GAMMA(Z) = 2.465 +/- 0.020 GeV, the hadronic and leptonic partial widths
GAMMA(h) = 1.726 +/- 0.019 GeV, GAMMA(t) = 83.4 +/- 0.8 MeV, the
invisible width GAMMA(inv) = 488 +/- 17 MeV, the ratio of hadronic over
leptonic partial widths R(Z)z = 20.70 +/- 0.29 and the Born level
hadronic peak cross section sigma-0 = 41.84 +/- 0.45 nb. A
flavour-independent measurement of the leptonic cross section gives very
consistent results to those presented above (GAMMA(t) = 83.7 +/- 0.8
MeV). From these results the number of light neutrino species is
determined to be N(nu) = 2.94 +/0. 10. The individual leptonic widths
obtained are: GAMMA(e) = 82.4 +/- 1.2 MeV, GAMMA(mu) = 86.9 +/- 2.1 MeV
and GAMMA(tau) = 82.7 +/- 2.4 MeV. Assuming universality, the squared
vector and axial-vector couplings of the Z0 to charged leptons are:
VBAR(t)2 = 0.0003 +/- 0.0010 and ABAR(l)2 = 0.2508 +/- 0.0027. These
values correspond to the electroweak parameters: rho(eff) = 1.003 +/-
0.011 and sin2-theta(W)eff = 0.241 +/- 0.009. Within the Minimal
Standard Model (MSM), the results can be expressed in terms of a single
parameter: sin2-theta(W)MSBAR = 0.2338 +/- 0.0027. All these values are
in good agreement with the predictions of the MSM. Fits yield 43 <
m(top) < 215 GeV at the 95% level. Finally, the measured values of
GAMMA(Z) and GAMMA(inv), are used to derive lower mass bounds for
possible new particles