26 research outputs found
Search for eccentric black hole coalescences during the third observing run of LIGO and Virgo
- Author
- Abac A.G.
- Abbott R.
- Abe H.
- Acernese F.
- Ackley K.
- Adamcewicz C.
- Adhicary S.
- Adhikari N.
- Adhikari R.X.
- Adkins V.K.
- Adya V.B.
- Affeldt C.
- Agarwal D.
- Agathos M.
- Aguiar O.D.
- Aguilar I.
- Aiello L.
- Ain A.
- Ajith P.
- Akutsu T.
- Al-Jodah A.
- Albanesi S.
- Alfaidi R.A.
- Allocca A.
- Alléné C.
- Almualla M.
- Altin P.A.
- Amato A.
- Amez-Droz L.
- Amorosi A.
- Anand S.
- Ananyeva A.
- Andersen R.
- Anderson S.B.
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- Andres N.
- Andrić T.
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- Apostolatos T.
- Appavuravther E.Z.
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- Yuzurihara H.
- Zadrożny A.
- Zannelli A.J.
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- Zeeshan M.
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- Zhu Z.-H.
- Zimmerman A.B.
- Zucker M.E.
- Zweizig J.
- Álvarez-López S.
- Publication venue
- American Astronomical Society
- Publication date
- 01/10/2024
- Field of study
Despite the growing number of binary black hole coalescences confidently observed through gravitational waves so far, the astrophysical origin of these binaries remains uncertain. Orbital eccentricity is one of the clearest tracers of binary formation channels. Identifying binary eccentricity, however, remains challenging due to the limited availability of gravitational waveforms that include the effects of eccentricity. Here, we present observational results for a waveform-independent search sensitive to eccentric black hole coalescences, covering the third observing run (O3) of the LIGO and Virgo detectors. We identified no new high-significance candidates beyond those that have already been identified with searches focusing on quasi-circular binaries. We determine the sensitivity of our search to high-mass (total source-frame mass M > 70 M⊙) binaries covering eccentricities up to 0.3 at 15 Hz emitted gravitational-wave frequency, and use this to compare model predictions to search results. Assuming all detections are indeed quasi-circular, for our fiducial population model, we place a conservative upper limit for the merger rate density of high-mass binaries with eccentricities 0 < e ≤ 0.3 at 16.9 Gpc−3 yr−1 at the 90% confidence level
Ultrasonic Synthetic Aperture Focusing Using the Root-Mean-Square Velocity
- Author
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Single gas chromatography method with nitrogen phosphorus detector for urinary cotinine determination in passive and active smokers
- Author
- ABU-QARE A.W.
- BECKETT A.H.
- BENOWITZ N.L.
- CHADWICK C.A.
- COPE G.
- DOCTOR P.B.
- FEYERABEND C.
- HAGAN R.L.
- HANSEN A.M.
- HARIHARAN M.
- HAUFROID V.
- Isarita Martins
- JARVIS M.J.
- JI JR A.
- KOLONEN S.A.
- KOWALSKI P.
- KUO H.W.
- Lusiane Malafatti
- MAN C.H.
- Maria Elisa Pereira Bastos de Siqueira
- Matheus Coutinho Gonçalves Martins
- MEGER M.
- MORIYA F.
- MOYER T.P.
- ODDOZE C.
- Patrícia Penido Maia
- QUEIROZ S.C.N
- RICHARD R.B.
- SHIN H.S.
- SONG L.
- TUOMI T.
- TYRPIEN K.
- VACCHINO M.N.
- VONCKEN P.
- WALL M.A.
- XU X.
- ZUCCARO P.
- Publication venue
- Universidade de São Paulo
- Publication date
- 01/12/2010
- Field of study
Nicotine is a major addictive compound in cigarettes and is rapidly and extensively metabolized to several metabolites in humans, including urinary cotinine, considered a biomarker due to its high concentration compared to other metabolites. The aim of this study was to develop a single method for determination of urinary cotinine, in active and passive smokers, by gas chromatography with a nitrogen phosphorus detector (GC-NPD). Urine (5.0 mL) was extracted with 1.0 mL of sodium hydroxide 5 mol L-1, 5.0 mL of chloroform, and lidocaine used as the internal standard. Injection volume was 1 μL in GC-NPD. Limit of quantification was 10 ng mL-1. Linearity was evaluated in the ranges 10-1000 ng mL-1 and 500-6000 ng mL-1, with determination coefficients of 0.9986 and 0.9952, respectively. Intra- and inter-assay standard relative deviations were lower than 14.2 %, while inaccuracy (bias) was less than +11.9%. The efficiency of extraction was greater than 88.5%. Ruggedness was verified, according to Youden's test. Means of cotinine concentrations observed were 2,980 ng mL-1 for active smokers and 132 ng mL-1, for passive smokers. The results revealed that satisfactory chromatographic separation between the analyte and interferents was obtained with a ZB-1 column. This method is reliable, precise, linear and presented ruggedness in the range evaluated. The results suggest that it can be applied in routine analysis for passive and active smokers, since it is able to quantify a wide range of cotinine concentrations in urine.<br>A nicotina é uma substância presente no cigarro capaz de causar dependência, sendo biotransformada em vários metabólitos nos seres humanos, dentre eles a cotinina urinária, que é considerada um indicador biológico de exposição à nicotina, devido a suas altas concentrações, comparado a outras matrizes. Assim, o objetivo deste estudo foi desenvolver um único método para determinação de cotinina urinária, em amostras de urina de fumantes ativos e passivos, através de cromatografia em fase gasosa com detector de nitrogênio- fósforo (CG-DNF). Para o preparo de amostras foram utilizados 5 mL de urina, 1 mL de hidróxido de sódio 5 mol L-1, 5 mL de clorofórmio, tendo como padrão interno a lidocaína. Na faixa de concentrações de 10-1000 ng mL-1 e 500- 6000 ng mL-1, o coeficiente de determinação foi 0,9986 e 0,9952, respectivamente e, o limite de quantificação foi 10 ng mL-1. A precisão intra- e interensaio apresentou desvio padrão relativo (%) menor que 14,2% e a inexatidão foi menor que +11,9%, com uma eficiência de extração de 88,5%. O método apresentou robustez, de acordo com o teste de Youden. As concentrações médias de cotinina observadas foram 2980 ng mL-1, para fumantes ativos e 132 ng mL-1, para fumantes passivos. Os resultados sugerem que o método é confiável, preciso, linear e apresentou robustez, na faixa avaliada, podendo ser aplicado na rotina para análises de amostras de fumantes ativos e passivos, pois é capaz de quantificar uma ampla faixa de concentrações de cotinina urinária
Passive Architectural Design Index applied to vernacular and passive buildings
- Author
- Ahuja R.
- Aini A.H.
- Ankit Kumar
- Building and Construction Authority
- Bureau of Energy Efficiency
- Bureau of Energy Efficiency
- Central Statistics office
- Charted Institution of Building Services Engineers
- Das N.
- Dhaka S.
- Doctor-Pingel M.
- Fanger P.O.
- Gontikaki M.
- Griha Manual Volume 3
- Gupta V.
- Indraganti M.
- International Energy Agency
- International Energy Agency
- Kanagaraj G.
- Krishan A.
- Kubota T.
- Larbi S.
- LEED-India N.C.
- Mofidi S.
- Nayak J.
- Neves L.
- Olgyay V.
- Phadke A.
- Pollock M.
- Priya R.S.
- Rodgers D.
- Scott A.
- Sriraj Gokarakonda
- Sundarraja M.
- Publication venue
- 'Informa UK Limited'
- Publication date
- Field of study
Biological activity of organotin compounds—An overview
- Author
- A.H. Penninks
- Alajouanine
- Aldridge
- Aldridge
- Aldridge
- Aldridge
- Ally
- Alzieu
- Barnes
- Barnes
- Barnes
- Beaumont
- Bentue-Ferrer
- Bierkamper
- Bouldin
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- Yaala M. Ben
- Yadav N
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- Yamamoto T.S
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- Yang Y
- Yarbrough Z
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- Yelikar A.B
- Yeung S.M.C
- Yin X
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- Yoo J
- Yu H
- Yuzurihara H
- Zadrożny A
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- Zanolin M
- Zeeshan M
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- Zevin M
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- Zhang T
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- Zhao Yue
- Zhao Yuhang
- Zheng Y
- Zhong H
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- Zhu Z.-H
- Zucker M.E
- Zweizig J
- Publication venue
- HAL CCSD
- Publication date
- 23/04/2024
- Field of study
International audienceAmong the various candidates for dark matter (DM), ultralight vector DM can be probed by laser interferometric gravitational wave detectors through the measurement of oscillating length changes in the arm cavities. In this context, KAGRA has a unique feature due to differing compositions of its mirrors, enhancing the signal of vector DM in the length change in the auxiliary channels. Here we present the result of a search for U(1)B−L gauge boson DM using the KAGRA data from auxiliary length channels during the first joint observation run together with GEO600. By applying our search pipeline, which takes into account the stochastic nature of ultralight DM, upper bounds on the coupling strength between the U(1)B−L gauge boson and ordinary matter are obtained for a range of DM masses. While our constraints are less stringent than those derived from previous experiments, this study demonstrates the applicability of our method to the lower-mass vector DM search, which is made difficult in this measurement by the short observation time compared to the auto-correlation time scale of DM
Ultralight vector dark matter search using data from the KAGRA O3GK run
- Author
- Abac A.G
- Abbott R
- Abe H
- Abouelfettouh I
- Acernese F
- Ackley K
- Adamcewicz C
- Adhicary S
- Adhikari N
- Adhikari R.X
- Adkins V.K
- Adya V.B
- Affeldt C
- Agarwal D
- Agathos M
- Aguiar O.D
- Aguilar I
- Aiello L
- Ain A
- Ajith P
- Akutsu T
- Al-Jodah A
- Al-Shammari S
- Albanesi S
- Alfaidi R.A
- Allocca A
- Alléné C
- Altin P.A
- Alvarez-Lopez S
- Amato A
- Amez-Droz L
- Amorosi A
- Amra C
- Anand S
- Ananyeva A
- Anderson S.B
- Anderson W.G
- Andia M
- Ando M
- Andrade T
- Andres N
- Andrić T
- Andrés-Carcasona M
- Anglin J
- Ansoldi S
- Antelis J.M
- Antier S
- Aoumi M
- Appavuravther E.Z
- Appert S
- Apple S.K
- Arai K
- Araya A
- Araya M.C
- Areeda J.S
- Arellano F.E. Peña
- Argianas L. Granda
- Aritomi N
- Armato F
- Arnaud N
- Arogeti M
- Aronson S.M
- Arun K.G
- Ashton G
- Aso Y
- Assiduo M
- Aston S.M
- Astone P
- Aubin F
- Aultoneal K
- Avallone G
- Babak S
- Badaracco F
- Badger C
- Bae S
- Bagnasco S
- Bagui E
- Bai Y
- Baier J.G
- Bajpai R
- Baka T
- Ball M
- Ballardin G
- Ballmer S.W
- Banagiri S
- Banerjee B
- Bankar D
- Baral P
- Barayoga J.C
- Barish B.C
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- Yaala M. Ben
- Yadav N
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- Yamamoto T.S
- Yamamura S
- Yamazaki R
- Yan S
- Yan T
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- Yang F.W
- Yang K.Z
- Yang L.-C
- Yang Y
- Yarbrough Z
- Yeh S.-W
- Yelikar A.B
- Yeung S.M.C
- Yin X
- Yokoyama J
- Yokozawa T
- Yoo J
- Yu H
- Yuzurihara H
- Zadrożny A
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- Zanolin M
- Zeeshan M
- Zelenova T
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- Zevin M
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- Zhao Yuhang
- Zheng Y
- Zhong H
- Zhong S
- Zhou R
- Zhu Z.-H
- Zucker M.E
- Zweizig J
- Publication venue
- HAL CCSD
- Publication date
- 23/04/2024
- Field of study
International audienceAmong the various candidates for dark matter (DM), ultralight vector DM can be probed by laser interferometric gravitational wave detectors through the measurement of oscillating length changes in the arm cavities. In this context, KAGRA has a unique feature due to differing compositions of its mirrors, enhancing the signal of vector DM in the length change in the auxiliary channels. Here we present the result of a search for U(1)B−L gauge boson DM using the KAGRA data from auxiliary length channels during the first joint observation run together with GEO600. By applying our search pipeline, which takes into account the stochastic nature of ultralight DM, upper bounds on the coupling strength between the U(1)B−L gauge boson and ordinary matter are obtained for a range of DM masses. While our constraints are less stringent than those derived from previous experiments, this study demonstrates the applicability of our method to the lower-mass vector DM search, which is made difficult in this measurement by the short observation time compared to the auto-correlation time scale of DM
Observation of Gravitational Waves from the Coalescence of a 2.5−4.5 M⊙ Compact Object and a Neutron Star
- Author
- Abac A.G
- Abbott R
- Abchouyeh M. Aghaei
- Abouelfettouh I
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- Ackley K
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- Adhikari R.X
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- Akçay S
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- Al-Shammari S
- Albanesi S
- Alfaidi R.A
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- Amra C
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- Anderson W.G
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- Washimi T
- Washington N.Y
- Watarai D
- Wayt K.E
- Weaver B
- Weaver B.R
- Weaving C.R
- Webster S.A
- Weinert M
- Weinstein A.J
- Weiss R
- Wellmann F
- Wen L
- Wette K
- Weßels P
- Whelan J.T
- Whiting B.F
- Whittle C
- Wildberger J.B
- Wilk O.S
- Wilken D
- Wilkin A.T
- Willadsen D.J
- Willetts K
- Williams D
- Williams M.J
- Williams N.S
- Willis J.L
- Willke B
- Wils M
- Winterflood J
- Wipf C.C
- Woan G
- Woehler J
- Wofford J.K
- Wolfe N.E
- Wong H.T
- Wong H.W.Y
- Wong I.C.F
- Wright J.L
- Wright M
- Wu C
- Wu D.S
- Wu H
- Wuchner E
- Wysocki D.M
- Xu V.A
- Xu Y
- Yaala M. Ben
- Yadav N
- Yamamoto H
- Yamamoto K
- Yamamoto T
- Yamamoto T.S
- Yamamura S
- Yamazaki R
- Yan S
- Yan T
- Yang F
- Yang F.W
- Yang K.Z
- Yang Y
- Yarbrough Z
- Yasui H
- Yeh S.-W
- Yelikar A.B
- Yin X
- Yokoyama J
- Yokozawa T
- Yoo J
- Yu H
- Yuan S
- Yuzurihara H
- Zadrożny A
- Zanolin M
- Zeeshan M
- Zelenova T
- Zendri J.-P
- Zeoli M
- Zerrad M
- Zevin M
- Zhang A.C
- Zhang L
- Zhang R
- Zhang T
- Zhang Y
- Zhao C
- Zhao Yue
- Zhao Yuhang
- Zheng Y
- Zhong H
- Zhou R
- Zhu X.-J
- Zhu Z.-H
- Zimmerman A.B
- Zucker M.E
- Zweizig J
- Publication venue
- HAL CCSD
- Publication date
- 01/01/2024
- Field of study
International audienceWe report the observation of a coalescing compact binary with component masses 2.5−4.5 M⊙ and 1.2−2.0 M⊙ (all measurements quoted at the 90% credible level). The gravitational-wave signal GW230529_181500 was observed during the fourth observing run of the LIGO-Virgo-KAGRA detector network on 2023 May 29 by the LIGO Livingston Observatory. The primary component of the source has a mass less than 5 M⊙ at 99% credibility. We cannot definitively determine from gravitational-wave data alone whether either component of the source is a neutron star or a black hole. However, given existing estimates of the maximum neutron star mass, we find the most probable interpretation of the source to be the coalescence of a neutron star with a black hole that has a mass between the most massive neutron stars and the least massive black holes observed in the Galaxy. We estimate a merger rate density of 55−47+127 Gpc−3yr−1 for compact binary coalescences with properties similar to the source of GW230529_181500; assuming that the source is a neutron star-black hole merger, GW230529_181500-like sources constitute about 60% of the total merger rate inferred for neutron star-black hole coalescences. The discovery of this system implies an increase in the expected rate of neutron star-black hole mergers with electromagnetic counterparts and provides further evidence for compact objects existing within the purported lower mass gap