recoil wave - PMC

Tristan Cullom, Cody Lough, Nicholas Altese, Douglas Bristow, Robert Landers, Ben Brown, Troy Hartwig, Andrew Barnard, Jason Blough, Kevin Johnson, Edward Kinzel

Sci Rep. 2021; 11: 10959. Published online 2021 May 26. doi: 10.1038/s41598-021-90423-z

PMCID:: PMC8155142

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Electromagnetic counterparts to massive black-hole mergers

Tamara Bogdanović, M. Coleman Miller, Laura Blecha

Living Rev Relativ. 2022; 25(1): 3. Published online 2022 Jun 24. doi: 10.1007/s41114-022-00037-8

PMCID:: PMC9232481

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Extremely fast feeding strikes are powered by elastic recoil in a seahorse relative, the snipefish, Macroramphosus scolopax

Sarah J. Longo, Tyler Goodearly, Peter C. Wainwright

Proc Biol Sci. 2018 Jul 11; 285(1882): 20181078. Published online 2018 Jul 4. doi: 10.1098/rspb.2018.1078

PMCID:: PMC6053929

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After wounding, a G-protein coupled receptor promotes the restoration of tension in epithelial cells

Ivy Han, Junmin Hua, James S. White, James T. O’Connor, Lila S. Nassar, Kaden J. Tro, Andrea Page-McCaw, M. Shane Hutson

Version 2. bioRxiv. Preprint. 2023 Jun 3 [revised 2024 Feb 18]. doi: 10.1101/2023.05.31.543122

Published in:: Mol Biol Cell. 2024 Mar 27 : mbcE23050204.

PMCID:: PMC10312550

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Attosecond interferometry of shape resonances in the recoil frame of CF₄

Saijoscha Heck, Denitsa Baykusheva, Meng Han, Jia-Bao Ji, Conaill Perry, Xiaochun Gong, Hans Jakob Wörner

Sci Adv. 2021 Dec; 7(49): eabj8121. Published online 2021 Dec 3. doi: 10.1126/sciadv.abj8121

PMCID:: PMC8641934

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Elastic recoil action amplifies jaw closing speed in an aquatic feeding salamander

Mateo Rull, Jacob Solomon, Nicolai Konow

Proc Biol Sci. 2020 May 27; 287(1927): 20200428. Published online 2020 May 20. doi: 10.1098/rspb.2020.0428

PMCID:: PMC7287362

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Dispersive-wave induced noise limits in miniature soliton microwave sources

Qi-Fan Yang, Qing-Xin Ji, Lue Wu, Boqiang Shen, Heming Wang, Chengying Bao, Zhiquan Yuan, Kerry Vahala

Nat Commun. 2021; 12: 1442. Published online 2021 Mar 4. doi: 10.1038/s41467-021-21658-7

PMCID:: PMC7933157

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New avenues for matter-wave-enhanced spectroscopy

Jonas Rodewald, Philipp Haslinger, Nadine Dörre, Benjamin A. Stickler, Armin Shayeghi, Klaus Hornberger, Markus Arndt

Appl Phys B. 2017; 123(1): 3. Published online 2016 Dec 9. doi: 10.1007/s00340-016-6573-y

PMCID:: PMC5148790

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Numerical simulation and experiment of double chamber brake based on CFD

Liu Yuhao, Qu Pu, Li Qiang

Sci Rep. 2023; 13: 17785. Published online 2023 Oct 18. doi: 10.1038/s41598-023-45010-9

PMCID:: PMC10584826

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Measurement, Analysis and Interpretation of Pressure/Flow Waves in Blood Vessels

Jonathan P. Mynard, Avinash Kondiboyina, Remi Kowalski, Michael M. H. Cheung, Joseph J. Smolich

Front Physiol. 2020; 11: 1085. Published online 2020 Aug 27. doi: 10.3389/fphys.2020.01085

PMCID:: PMC7481457

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Attosecond photoionisation time delays reveal the anisotropy of the molecular potential in the recoil frame

H. Ahmadi, E. Plésiat, M. Moioli, F. Frassetto, L. Poletto, P. Decleva, C. D. Schröter, T. Pfeifer, R. Moshammer, A. Palacios, F. Martin, G. Sansone

Nat Commun. 2022; 13: 1242. Published online 2022 Mar 10. doi: 10.1038/s41467-022-28783-x

PMCID:: PMC8913798

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Tunneling gravimetry

Patrik Schach, Alexander Friedrich, Jason R. Williams, Wolfgang P. Schleich, Enno Giese

EPJ Quantum Technol. 2022; 9(1): 20. Published online 2022 Aug 2. doi: 10.1140/epjqt/s40507-022-00140-3

PMCID:: PMC9345841

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In vivo assessment of stent recoil of biodegradable polymer-coated cobalt–chromium sirolimus-eluting coronary stent system

Atul D. Abhyankar, Ashok S. Thakkar

Indian Heart J. 2012 Nov; 64(6): 541–546. doi: 10.1016/j.ihj.2012.07.005

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Single-mode dispersive waves and soliton microcomb dynamics

Xu Yi, Qi-Fan Yang, Xueyue Zhang, Ki Youl Yang, Xinbai Li, Kerry Vahala

Nat Commun. 2017; 8: 14869. Published online 2017 Mar 23. doi: 10.1038/ncomms14869

PMCID:: PMC5376647

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Feshbach enhanced s-wave scattering of fermions: direct observation with optimized absorption imaging

D Genkina, LM Aycock, BK Stuhl, H-I Lu, RA Williams, IB Spielman

New J Phys. Author manuscript; available in PMC 2017 Jan 1.

Published in final edited form as: New J Phys. 2016 Jan; 18: 013001. Published online 2015 Dec 17. doi: 10.1088/1367-2630/18/1/013001

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Neuromechanical wave resonance in jellyfish swimming

Alexander P. Hoover, Nicole W. Xu, Brad J. Gemmell, Sean P. Colin, John H. Costello, John O. Dabiri, Laura A. Miller

Proc Natl Acad Sci U S A. 2021 Mar 16; 118(11): e2020025118. Published online 2021 Mar 8. doi: 10.1073/pnas.2020025118

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Recoil effects of a motional scatterer on single-photon scattering in one dimension

Qiong Li, D. Z. Xu, C. Y. Cai, C. P. Sun

Sci Rep. 2013; 3: 3144. Published online 2013 Nov 13. doi: 10.1038/srep03144

PMCID:: PMC3826102

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Arterial pulse wave modeling and analysis for vascular-age studies: a review from VascAgeNet

Jordi Alastruey, Peter H. Charlton, Vasiliki Bikia, Birute Paliakaite, Bernhard Hametner, Rosa Maria Bruno, Marijn P. Mulder, Samuel Vennin, Senol Piskin, Ashraf W. Khir, Andrea Guala, Christopher C. Mayer, Jonathan Mynard, Alun D. Hughes, Patrick Segers, Berend E. Westerhof

Am J Physiol Heart Circ Physiol. 2023 Jul 1; 325(1): H1–H29. Published online 2023 Mar 31. doi: 10.1152/ajpheart.00705.2022

PMCID:: PMC7614613

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FIG. 1

Energy levels and matter-optical energy-momentum conservation. (a) Energy level diagram with laser coupling for three-photon hyper-Raman generation. (b) Colinear pumping geometry for the backward generation of hyper-Raman mixing wave. (c) Wave vector diagram showing combined matter-optical wave phase matching. Optical wave vector and energy mismatch are given by Δk⃗ = 3k⃗_L − k⃗_M and Δω = 3ω_L − ω_M. The atomic quasimomentum and total recoil energy are ħq⃗ and ħω_R = (ħq)²/(2M).

Matter-Wave–Optical-Wave Mixing-Induced Transparency and a Nonhyperbolic Matter-Wave Quasisoliton in Quantum Gases

Phys Rev Lett. ;118(1):013901-013901.
Fig. 2Distribution NJ(αkR) over J in the rotational recoil-induced wave packet for different αkR. The red squares in the insert show the dependence of Jmax on the recoil angular momentum αkR. Here Jmax is the value of the angular momentum J when the distribution NJ(αkR) takes maximum. The dashed diagonal line in the insert corresponds to the recoil angular momentum Jrec = αkR (6).

Time-resolved study of recoil-induced rotation by X-ray pump – X-ray probe spectroscopy

Phys Chem Chem Phys. 2022 Mar 16;24(11):6627-6638.
Figure 4.

(a). When the ventricle contracts, the semilunar valve opens. Blood ejects into the aorta and arteries and makes them expanded. At the same time, the pressure stores in the elastic walls. This percussion produces the P wave. (b). Isovolumic ventricular relaxation makes the semilunar valve shut. Elastic recoil of arteries sends blood forward into the rest of circulatory system. This rebound makes the T wave and the closing of valve makes the D wave.

Variation Analysis of Sphygmogram to Assess Cardiovascular System under Meditation

Evid Based Complement Alternat Med. 2009 Mar;6(1):107-112.
Figure 4The geometrical scalar potential W(z) created by a plane wave, in units of the energy recoil , as a function of z for two different angles of incidence θ − θ0 = 8 · 10−4 rad (solid black line), θ − θ0 = 10−5 rad (dashed red line) and for s = 5, see Eq. (9), and λ = 578 nm.

Artificial magnetic field induced by an evanescent wave

Sci Rep. 2015;5:7672.