2,898 research outputs found
A literature review on surgery for cervical vagal schwannomas
- Author
- A Peyvandi
- A Ziadi
- AL Moroni
- BK Lahoti
- D Biswas
- E Langner
- EN Callum
- GC Kang
- Giada Pattaro
- Gianfranco Silecchia
- Giuseppe Cavallaro
- H Liu
- J Valentino
- JL Roh
- KC Chiun
- KR Hwang
- L Rogers
- Marcello Avallone
- MG Chiofalo
- MJ Gibber
- MK Bhayani
- MR Sreevatsa
- NG McGuire
- Olga Iorio
- R Bilancia
- R Matsuo
- R Yasumatsu
- RI RĂźckert
- RM Lee
- RS Murley
- SH Kim
- T Ogawa
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2015
- Field of study
Cervical vagal schwannoma is a benign, slow-growing mass, often asymptomatic, with a very low lifetime risk of malignant transformation in general population, but diagnosis is still a challenge. Surgical resection is the treatment of choice even if its close relationship with nerve fibres, from which it arises, threats vagal nerve preservation. We present a case report and a systematic review of literature. All studies on surgical resection of cervical vagal schwannoma have been reviewed. Papers matching the inclusion criteria (topic on surgical removal of cervical vagal schwannoma, English language, full text available) were selected. Fifty-three patients with vagal neck schwannoma submitted to surgery were identified among 22 studies selected. Female/male ratio was 1.5 and median age 44 years. Median diameter was 5 cm (range 2 to 10). Most schwannoma were asymptomatic (68.2%) and received an intracapsular excision (64.9%). Postoperative symptoms were reported in 22.6% of patients. Cervical vagal schwannoma is a benign pathology requiring surgical excision, but frequently postoperative complications can affect patients lifelong, so, surgical indications should be based carefully on the balance between risks and benefits
Insects as Stem Engineers: Interactions Mediated by the Twig-Girdler Oncideres albomarginata chamela Enhance Arthropod Diversity
- Author
- A Hastings
- AJ MartĂnez
- AM Waltz
- BD Duval
- BH Aukema
- C Uribe-MĂş
- CG Jones
- CS Awmack
- D Tilman
- DP Faith
- DS Srivastava
- EAJ Duffy
- EJ Gerberg
- F Binda
- F Forcella
- F Lieutier
- FA Noguera
- FT Hovore
- GD Amman
- GD Martinsen
- GD Martinsen
- Guy Smagghe
- H Damman
- H Kagata
- IC Feller
- IC Feller
- IC Feller
- J Helbig
- JA Chemsak
- JE Byers
- JJ Stachowicz
- JP Wright
- JT Lill
- KL Polk
- LM Hanks
- Luis H. Escalera-VĂĄzquez
- M Kenis
- M RamĂrez-MartĂnez
- MA Equihua
- Mauricio Quesada
- ME Power
- MJ Maass
- N CalderĂłn-CortĂŠs
- Nancy CalderĂłn-CortĂŠs
- NG Hairston
- NJ Gotelli
- NJ Gotelli
- OR Di Iorio
- P Daleo
- PA Abrams
- PJ Johnson SN Mayhew
- PJ Morin
- RC Littell
- RH Arnett
- RJ Marquis
- RT Paine
- S Nylin
- S Utsumi
- SH Bullock
- SH Bullock
- SH Bullock
- T Ohgushi
- TD Schowalter
- WR Rice
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2011
- Field of study
Background: Ecosystem engineering may influence community structure and biodiversity by controlling the availability of resources and/or habitats used by other organisms. Insect herbivores may act as ecosystem engineers but there is still poor understanding of the role of these insects structuring arthropod communities. Methodology/Principal Findings: We evaluated the effect of ecosystem engineering by the stem-borer Oncideres albomarginata chamela on the arthropod community of a tropical dry forest for three consecutive years. The results showed that ecosystem engineering by O. albomarginata chamela had strong positive effects on the colonization, abundance, species richness and composition of the associated arthropod community, and it occurred mainly through the creation of a habitat with high availability of oviposition sites for secondary colonizers. These effects cascade upward to higher trophic levels. Overall, ecosystem engineering by O. albomarginata chamela was responsible for nearly 95 % of the abundance of secondary colonizers and 82 % of the species richness. Conclusions/Significance: Our results suggest that ecosystem engineering by O. albomarginata chamela is a keystone process structuring an arthropod community composed by xylovores, predators and parasitoids. This study is the first to empirically demonstrate the effect of the ecosystem engineering by stem-boring insects on important attributes o
Taurine: a potential marker of apoptosis in gliomas
- Author
- A Moreno-Torres
- B A Bell
- C RĂŠmy
- CL Wu
- E Iorio
- EJ Delikatny
- F A Howe
- F Lang
- H Lahrech
- H Lei
- H Lyng
- J MorĂĄn
- J R Griffiths
- JE Schmitz
- JL Griffin
- JM Hakumäki
- JP Usenius
- K S Opstad
- KS Opstad
- KS Opstad
- KS Opstad
- LL Cheng
- M Di Vito
- M GĂłmez-Angelats
- M Milkevitch
- M Watanabe
- MB Friis
- NM Al-Saffar
- R Gold
- RD Rao
- S Zoula
- SH Kaufmann
- TL Perry
- V Govindaraju
- Y Gavrieli
- Publication venue
- Nature Publishing Group
- Publication date
- 17/02/2009
- Field of study
New cancer therapies are being developed that trigger tumour apoptosis and an in vivo method of apoptotic detection and early treatment response would be of great value. Magnetic resonance spectroscopy (MRS) can determine the tumour biochemical profile in vivo, and we have investigated whether a specific spectroscopic signature exists for apoptosis in human astrocytomas. High-resolution magic angle spinning (HRMAS) 1H MRS provided detailed 1H spectra of brain tumour biopsies for direct correlation with histopathology. Metabolites, mobile lipids and macromolecules were quantified from presaturation HRMAS 1H spectra acquired from 41 biopsies of grades II (n=8), III (n=3) and IV (n=30) astrocytomas. Subsequently, TUNEL and H&E staining provided quantification of apoptosis, cell density and necrosis. Taurine was found to significantly correlate with apoptotic cell density (TUNEL) in both non-necrotic (R=0.727, P=0.003) and necrotic (R=0.626, P=0.0005) biopsies. However, the ca 2.8âp.p.m. polyunsaturated fatty acid peak, observed in other studies as a marker of apoptosis, correlated only in non-necrotic biopsies (R=0.705, P<0.005). We suggest that the taurine 1H MRS signal in astrocytomas may be a robust apoptotic biomarker that is independent of tumour necrotic status
Performance of CMS muon reconstruction in pp collision events at sqrt(s) = 7 TeV
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Acosta D
- Acosta JG
- Acosta MV
- Adair A
- Adam N
- Adam W
- Adams MR
- Adams T
- Adiguzel A
- Adler V
- Adzic P
- Agostino L
- Agram JL
- Aguilar-Benitez M
- Aguilo E
- Ahmad M
- Ahmad WH
- Ahuja S
- Akchurin N
- Akgun B
- Akgun U
- Akin IV
- Alagoz E
- Albajar C
- Albayrak EA
- Albergo S
- Albrow M
- Alda Junior WL
- Alexander J
- Aliev T
- Almeida N
- Alver B
- Alverson G
- Alves GA
- Amapane N
- Amsler C
- Anagnostou G
- Anastassov A
- Anderson J
- Anderson M
- Andrea J
- Andreev V
- Andreev V
- Andreev Y
- Andrews W
- Anghel IM
- Anjos TS
- Antonelli L
- Antunes JR
- Antunovic Z
- Apanasevich L
- Apollinari G
- Appelt E
- Apresyan A
- Aranyi A
- Arce P
- Arcidiacono R
- Arenton MW
- Arfaei H
- Argiro S
- Arisaka K
- Arneodo M
- Arora S
- Asawatangtrakuldee C
- Asghar MI
- Askew A
- Assran Y
- Ata M
- Atac M
- Atramentov O
- Attikis A
- Auffray E
- Autermann C
- Auzinger G
- Avdeeva E
- Avery P
- Avetisyan A
- Azarkin M
- Azhgirey I
- Aziz T
- Azzi P
- Azzolini V
- Azzurri P
- Baarmand MM
- Babb J
- Bacchetta N
- Bachtis M
- Baden A
- Baeni L
- Baesso P
- Baffioni S
- Bagliesi G
- Bai Y
- Baillon P
- Bainbridge R
- Bakhshiansohi H
- Bakirci MN
- Bakken JA
- Balazs M
- Ball AH
- Ball G
- Ban Y
- Banerjee S
- Banerjee S
- Bansal S
- Banzuzi K
- Barbagli G
- Barberis E
- Barbone L
- Bardak C
- Barfuss AF
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- Barge D
- Baringer P
- Barker A
- Barnes VE
- Barnett BA
- Barney D
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- Barrett M
- Bartalini P
- Barth C
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- Basso L
- Battilana C
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- Bauer G
- Bauerdick LAT
- Baumgartel D
- Baur U
- Bayshev I
- Bazterra VE
- Bean A
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- Beaudette F
- Beaupere N
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- Waltenberger W
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- Wardrope D
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- Weiler T
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- Xiao H
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- Yazgan E
- Yelton J
- Yetkin T
- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoo J
- Yoon AS
- York A
- Yu I
- Yu SS
- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
- Zang SL
- Zarubin A
- Zatserklyaniy A
- Zeinali M
- Zeise M
- Zeuner WD
- Zeyrek M
- Zhang J
- Zhang Z
- Zheng Y
- Zhokin A
- Zhu B
- Zhu RY
- Zhukov V
- Zhukova V
- Ziebarth EB
- Ziegler J
- Zielinski M
- Zito G
- Zoeller MH
- Zotto P
- Zou W
- Zumerle G
- Zuranski A
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2012
- Field of study
The performance of muon reconstruction, identification, and triggering in CMS
has been studied using 40 inverse picobarns of data collected in pp collisions
at sqrt(s) = 7 TeV at the LHC in 2010. A few benchmark sets of selection
criteria covering a wide range of physics analysis needs have been examined.
For all considered selections, the efficiency to reconstruct and identify a
muon with a transverse momentum pT larger than a few GeV is above 95% over the
whole region of pseudorapidity covered by the CMS muon system, abs(eta) < 2.4,
while the probability to misidentify a hadron as a muon is well below 1%. The
efficiency to trigger on single muons with pT above a few GeV is higher than
90% over the full eta range, and typically substantially better. The overall
momentum scale is measured to a precision of 0.2% with muons from Z decays. The
transverse momentum resolution varies from 1% to 6% depending on pseudorapidity
for muons with pT below 100 GeV and, using cosmic rays, it is shown to be
better than 10% in the central region up to pT = 1 TeV. Observed distributions
of all quantities are well reproduced by the Monte Carlo simulation.Comment: Replaced with published version. Added journal reference and DO
Constraints on the Ď_(c1) versus Ď_(c2) polarizations in proton-proton collisions at âs = 8 TeV
- Author
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- Zevi Della Porta G.
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- Zientek M.
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- Zolkapli Z.
- Zorbakir I.âS.
- Zorbilmez C.
- Zotto P.
- Zou D.
- Zucchetta A.
- Zumerle G.
- Zuo X.
- Zuolo D.
- Ălvarez FernĂĄndez A.
- Ăzçelik Ă.
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 24/04/2020
- Field of study
The polarizations of promptly produced Ď_(c1) and Ď_(c2) mesons are studied using data collected by the CMS experiment at the LHC, in proton-proton collisions at âs=8ââTeV. The Ď_c states are reconstructed via their radiative decays Ď_c â J/ĎÎł, with the photons being measured through conversions to eâşeâť, which allows the two states to be well resolved. The polarizations are measured in the helicity frame, through the analysis of the Ď_(c2) to Ď_(c1) yield ratio as a function of the polar or azimuthal angle of the positive muon emitted in the J/Ď â ÎźâşÎźâť decay, in three bins of J/Ď transverse momentum. While no differences are seen between the two states in terms of azimuthal decay angle distributions, they are observed to have significantly different polar anisotropies. The measurement favors a scenario where at least one of the two states is strongly polarized along the helicity quantization axis, in agreement with nonrelativistic quantum chromodynamics predictions. This is the first measurement of significantly polarized quarkonia produced at high transverse momentum
Performance of CMS muon reconstruction in pp collision events at sqrt(s) = 7 TeV
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- Shi X
- Shipkowski SP
- Shipsey I
- Shiu JG
- Shivpuri RK
- Shmatov S
- Shoaib M
- Shrestha S
- Shreyber I
- Shukla P
- Shumeiko N
- Sibille J
- Siegrist P
- Sierra RV
- Sigamani M
- Sikler F
- Silkworth C
- Sill A
- Sillou D
- Silva Do Amaral SM
- Silva P
- Silvers D
- Silverwood H
- Silvestre C
- Silvestris L
- Sim KS
- Simon M
- Simon S
- Simonetto F
- Simonis HJ
- Singh AP
- Singh G
- Singh J
- Singh SP
- Singovsky A
- Sinthuprasith T
- Sirois Y
- Siroli G
- Sirunyan AM
- Skhirtladze N
- Skuja A
- Slaunwhite J
- Smirnov I
- Smith J
- Smith JG
- Smith K
- Smith VJ
- Smith WH
- Smolin D
- Snigirev A
- Snoek H
- Snook B
- Snow GR
- Snowball M
- Soares Jorge L
- Soares MS
- Sobol A
- Sobron Sanudo M
- Soffi L
- Sogut K
- Sola V
- Solano A
- Somalwar S
- Son DC
- Song S
- Sonmez N
- Sonnenschein L
- Sordini V
- Souza MHG
- Spagnolo P
- Spalding WJ
- Spanier S
- Sparrow A
- Speer T
- Sperka D
- Sphicas P
- Spiegel L
- Spiga D
- Spiridonov A
- Spiropulu M
- Sprenger D
- Squires M
- Stadie H
- Stahl A
- Staiano A
- Starodumov A
- Steggemann J
- Stein M
- Steinbrueck G
- Stenson K
- Stephans GSF
- Stickland D
- Stieger B
- Stiliaris E
- Stober FM
- Stoeckli F
- Stolin V
- Stone R
- Stoye M
- Stoykova S
- Stoynev S
- Strauss J
- Stringer R
- Strobbe N
- Strom D
- Stuart D
- Sturdy J
- Suarez I
- Suarez RG
- Sudano E
- Sudhakar K
- Sulak L
- Sulimov V
- Sultanov G
- Summers D
- Sumorok K
- Sumowidagdo S
- Sun W
- Sung K
- Surat UE
- Svintradze I
- Svyatkovskiy A
- Swanson J
- Swartz M
- Symonds P
- Szillasi Z
- Szleper M
- Sznajder A
- Tadel M
- Takahashi M
- Tali B
- Tambe N
- Tan P
- Tao J
- Tapper A
- Taroni S
- Tatarinov A
- Taurok A
- Tauscher L
- Taylor L
- Tcholakov V
- Teischinger F
- Temple J
- Tenchini R
- Teng H
- Teo WD
- Teodorescu L
- Teyssier D
- Thea A
- Theofilatos K
- Thiebaux C
- Thom J
- Thomas L
- Thomas S
- Thompson J
- Thomsen J
- Thyssen F
- Tiko A
- Timciuc V
- Tinti G
- Tiras E
- Titov M
- Tkaczyk S
- To W
- Toback D
- Tomalin IR
- Tomaszewska J
- Tonelli G
- Tonjes MB
- Tonwar SC
- Topakli H
- Topaksu AK
- Torassa E
- Toropin A
- Torre P
- Tosi M
- Tosi S
- Tourneur S
- Tourtchanovitch L
- Traczyk P
- Tran NV
- Travaglini R
- Trayanov R
- Treille D
- Triantis FA
- Tricomi A
- Tripathi M
- Trocino D
- Trocsanyi ZL
- Troendle D
- Troitsky S
- Tropiano A
- Troshin S
- Tsang KV
- Tschudi Y
- Tsirou A
- Tu Y
- Tucker J
- Tully C
- Tumasyan A
- Tuo S
- Tuominen E
- Tuominiemi J
- Tuovinen E
- Tupputi S
- Turkewitz J
- Turner M
- Tuuva T
- Tuve C
- Twedt E
- Tytgat M
- Tyurin N
- Tzeng YM
- Ujvari B
- Ulmer KA
- Ungaro D
- Uplegger L
- Urscheler C
- Uvarov L
- Uzun D
- Uzunian A
- Vaandering EW
- Valdata M
- Valls N
- Valuev V
- Van Doninck W
- Van Haevermaet H
- Van Hove P
- Van Mechelen P
- Van Mulders P
- Van Onsem GP
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- Van Spilbeeck A
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- Vartak A
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- Vaughan J
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- Vazquez Valencia F
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- Villasenor-Cendejas LM
- Villella I
- Vinogradov A
- Virdee T
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- Vogel H
- Volkov A
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- Weber M
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- Weiler T
- Weinberg M
- Wendland L
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- Wenger EA
- Werner JS
- West C
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- Whyntie T
- Wickens J
- Wickramage N
- Widl E
- Wigmans R
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- Wilkinson R
- Williams G
- Williams T
- Willmott C
- Wimpenny S
- Winn D
- Winstrom L
- Wissing C
- Wittich P
- Wittmer B
- Woehri HK
- Wolf M
- Wolf R
- Womersley WJ
- Won S
- Wood D
- Wood J
- Wood JS
- Worm SD
- Wright D
- Wrochna G
- Wu W
- Wuerthwein F
- Wulz C-E
- Wyslouch B
- Xiao H
- Xie S
- Xu M
- Yagil A
- Yalvac M
- Yang F
- Yang M
- Yang Y
- Yang ZC
- Yazgan E
- Yelton J
- Yetkin T
- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoo J
- Yoon AS
- York A
- Yu I
- Yu SS
- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
- Zang SL
- Zarubin A
- Zatserklyaniy A
- Zeinali M
- Zeise M
- Zeuner WD
- Zeyrek M
- Zhang J
- Zhang Z
- Zheng Y
- Zhokin A
- Zhu B
- Zhu RY
- Zhukov V
- Zhukova V
- Ziebarth EB
- Ziegler J
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- Zoeller MH
- Zotto P
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- Zumerle G
- Zuranski A
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2012
- Field of study
The performance of muon reconstruction, identification, and triggering in CMS
has been studied using 40 inverse picobarns of data collected in pp collisions
at sqrt(s) = 7 TeV at the LHC in 2010. A few benchmark sets of selection
criteria covering a wide range of physics analysis needs have been examined.
For all considered selections, the efficiency to reconstruct and identify a
muon with a transverse momentum pT larger than a few GeV is above 95% over the
whole region of pseudorapidity covered by the CMS muon system, abs(eta) < 2.4,
while the probability to misidentify a hadron as a muon is well below 1%. The
efficiency to trigger on single muons with pT above a few GeV is higher than
90% over the full eta range, and typically substantially better. The overall
momentum scale is measured to a precision of 0.2% with muons from Z decays. The
transverse momentum resolution varies from 1% to 6% depending on pseudorapidity
for muons with pT below 100 GeV and, using cosmic rays, it is shown to be
better than 10% in the central region up to pT = 1 TeV. Observed distributions
of all quantities are well reproduced by the Monte Carlo simulation.Comment: Replaced with published version. Added journal reference and DO
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