Manipulation of solid-liquid interface of ⁴He by acoustic radiation pressure

Acoustic radiation pressure is thought to be very useful for solid ⁴He experiment under the microgravity. We observed that solid-liquid interface of ⁴He was manipulated by the acoustic wave. We applied the sound pulse perpendicularly to the flat interface between two transducers. The interface moved...

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Datum:2003
Hauptverfasser: Nomura, R., Suzuki, Y., Kimura, S., Okuda, Y., Burmistrov, S.
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Sprache:English
Veröffentlicht: Фізико-технічний інститут низьких температур ім. Б.І. Вєркіна НАН України 2003
Schriftenreihe:Физика низких температур
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Online Zugang:http://dspace.nbuv.gov.ua/handle/123456789/128855
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Zitieren:Manipulation of solid-liquid interface of ⁴He by acoustic radiation pressure / R. Nomura, Y. Suzuki, S. Kimura, Y. Okuda, S. Burmistrov // Физика низких температур. — 2003. — Т. 29, № 6. — С. 663-666. — Бібліогр.: 8 назв. — англ.

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spelling irk-123456789-1288552018-01-15T03:05:03Z Manipulation of solid-liquid interface of ⁴He by acoustic radiation pressure Nomura, R. Suzuki, Y. Kimura, S. Okuda, Y. Burmistrov, S. 3-й Международный семинар по физике низких температур в условиях микрогравитации Acoustic radiation pressure is thought to be very useful for solid ⁴He experiment under the microgravity. We observed that solid-liquid interface of ⁴He was manipulated by the acoustic wave. We applied the sound pulse perpendicularly to the flat interface between two transducers. The interface moved to the sound direction at low temperatures. We also checked how the interface moved when sound was applied parallel to the interface. Dynamics of the interface during and after the sound pulse were recorded by a high speed CCD camera. 2003 Article Manipulation of solid-liquid interface of ⁴He by acoustic radiation pressure / R. Nomura, Y. Suzuki, S. Kimura, Y. Okuda, S. Burmistrov // Физика низких температур. — 2003. — Т. 29, № 6. — С. 663-666. — Бібліогр.: 8 назв. — англ. 0132-6414 PACS: 67.80.-s, 81.10.-h, 43.35.+d http://dspace.nbuv.gov.ua/handle/123456789/128855 en Физика низких температур Фізико-технічний інститут низьких температур ім. Б.І. Вєркіна НАН України
institution Digital Library of Periodicals of National Academy of Sciences of Ukraine
collection DSpace DC
language English
topic 3-й Международный семинар по физике низких температур в условиях микрогравитации
3-й Международный семинар по физике низких температур в условиях микрогравитации
spellingShingle 3-й Международный семинар по физике низких температур в условиях микрогравитации
3-й Международный семинар по физике низких температур в условиях микрогравитации
Nomura, R.
Suzuki, Y.
Kimura, S.
Okuda, Y.
Burmistrov, S.
Manipulation of solid-liquid interface of ⁴He by acoustic radiation pressure
Физика низких температур
description Acoustic radiation pressure is thought to be very useful for solid ⁴He experiment under the microgravity. We observed that solid-liquid interface of ⁴He was manipulated by the acoustic wave. We applied the sound pulse perpendicularly to the flat interface between two transducers. The interface moved to the sound direction at low temperatures. We also checked how the interface moved when sound was applied parallel to the interface. Dynamics of the interface during and after the sound pulse were recorded by a high speed CCD camera.
format Article
author Nomura, R.
Suzuki, Y.
Kimura, S.
Okuda, Y.
Burmistrov, S.
author_facet Nomura, R.
Suzuki, Y.
Kimura, S.
Okuda, Y.
Burmistrov, S.
author_sort Nomura, R.
title Manipulation of solid-liquid interface of ⁴He by acoustic radiation pressure
title_short Manipulation of solid-liquid interface of ⁴He by acoustic radiation pressure
title_full Manipulation of solid-liquid interface of ⁴He by acoustic radiation pressure
title_fullStr Manipulation of solid-liquid interface of ⁴He by acoustic radiation pressure
title_full_unstemmed Manipulation of solid-liquid interface of ⁴He by acoustic radiation pressure
title_sort manipulation of solid-liquid interface of ⁴he by acoustic radiation pressure
publisher Фізико-технічний інститут низьких температур ім. Б.І. Вєркіна НАН України
publishDate 2003
topic_facet 3-й Международный семинар по физике низких температур в условиях микрогравитации
url http://dspace.nbuv.gov.ua/handle/123456789/128855
citation_txt Manipulation of solid-liquid interface of ⁴He by acoustic radiation pressure / R. Nomura, Y. Suzuki, S. Kimura, Y. Okuda, S. Burmistrov // Физика низких температур. — 2003. — Т. 29, № 6. — С. 663-666. — Бібліогр.: 8 назв. — англ.
series Физика низких температур
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AT suzukiy manipulationofsolidliquidinterfaceof4hebyacousticradiationpressure
AT kimuras manipulationofsolidliquidinterfaceof4hebyacousticradiationpressure
AT okuday manipulationofsolidliquidinterfaceof4hebyacousticradiationpressure
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fulltext Fizika Nizkikh Temperatur, 2003, v. 29, No. 6, p. 663–666 Manipulation of solid-liquid interface of 4He by acoustic radiation pressure R. Nomura, Y. Suzuki, S. Kimura, Y. Okuda, and S. Burmistrov* Department of Condensed Matter Physics, Tokyo Institute of Technology 2-12-1, O-okayama, Meguro-ku, Tokyo 152-8551, Japan E-mail: nomura@ap.titech.ac.jp Received December 19, 2002 Acoustic radiation pressure is thought to be very useful for solid 4He experiment under the microgravity. We observed that solid-liquid interface of 4He was manipulated by the acoustic wave. We applied the sound pulse perpendicularly to the flat interface between two transducers. The interface moved to the sound direction at low temperatures. We also checked how the inter- face moved when sound was applied parallel to the interface. Dynamics of the interface during and after the sound pulse were recorded by a high speed CCD camera. PACS: 67.80.–s, 81.10.–h, 43.35.+d Introduction In the microgravity environment it is very impor- tant to control an object without a direct contact. For this purpose acoustic radiation pressure is a useful tool. It was used for investigating the dynamics of li- quid drops [1,2] and for passive stabilization of liquid capillary bridges [3] in the low-gravity. In case of a crystal growth experiment under the microgravity it is not easy to keep and control the crystal at a proper position. Once it detaches from a wall and starts to move freely, it is very difficult to stop it especially in a superfluid that has no viscosity. It will be very helpful if one can control the motion of 4He crystal easily. This kind of technique will also be used to study new types of dynamics like a shape evo- lution of rotating quantum crystal under the microgravity, collision or friction between two quan- tum crystals and so on. Acoustic radiation pressure is thought to be a good way to manipulate the crystal. We found that solid-liquid interface of 4He, which is known to have an ultrahigh mobility [4,5], could be manipulated by sound wave. When the sound pulse was applied from the liquid side to the flat interface, the solid was melted at all temperatures below 1.2 K. But when the sound pulse was applied from the solid side the solid was melted above 750 mK and grown be- low it [6,7]. These interface motion were driven by acoustic radiation pressure. In quantum mechanical representations radiation pressure is interpreted as momentum transfer from phonons to the interface [8]. We recorded the dynamics of interface during and af- ter the sound pulse by a high-speed CCD camera. Experimental results and discussions Experiment was performed in a cell cooled by a di- lution refrigerator. It had optical access from room © R. Nomura, Y. Suzuki, S. Kimura, Y. Okuda, and S. Burmistrov, 2003 * Permanent address: Department of Superconductivity and Solid State Physics, Kurchatov Institute, Moscow 123182, Russia Fig. 1. Melting of 4He crystal induced by sound wave from the liquid side. temperature and we could observe 4He crystal down to 50 mK. Two longitudinal transducers faced each other were prepared in a cell. Their resonance fre- quency was about 10 MHz and distance was 10 mm. Sound directions were vertical. Large 4He crystal was grown in the cell and occupied the lower half space. Solid-liquid interface was adjusted midway between the two transducers. It was horizontally flat without sound because of the gravity. Sound pulse was applied to the interface from the liquid side or downward by the upper transducer and from the solid side or up- ward by the lower transducer. We also set up two other transducers. Sound direction of them was hori- zontal or parallel to the interface. One was for longi- tudinal sound and the other was for transverse sound. Figure 1 is the shape of a solid-liquid interface while sound wave was applied from the liquid side. Melting was induced at around the center of the cell where the sound wave was actually applied. Tempera- ture was about 150 mK and typical sound power den- sity for these figures was about 200 W/m2. When sound was applied from the solid side at the same tem- perature, the crystal was grown as shown in Fig. 2. So the interface was pushed to the direction of sound at these low temperatures. We could induce both crystal- lization and melting easily by changing the direction of acoustic wave. We also applied sound horizontally and checked how the interface responded to it. Sound direction was parallel to the interface in this case. Longitudinal sound was applied from left to right at around 150 mK and it stochastically induced melting (Fig. 3) or crys- tallization (Fig. 4) in the vicinity of the transducer. These observations support the idea that acoustic radi- ation pressure was the cause of the interface motion. The interface motion was driven not because solid or liquid were thermodynamically favored but because the interface felt the force directly from the sound wave. Initial tiny slope of the interface probably de- termined whether crystallization or melting was in- duced. When transverse sound was applied from right to left it always induced crystallization (Fig. 5) be- cause it can propagate only through the solid. Using a high-speed CCD camera interface dyna- mics were recorded during and after a sound pulse. Sound pulse of 1 msec duration was applied at t = 0 from the liquid side. First it induced downward mo- tion of the interface. Then the interface oscillated around the equilibrium position as shown in Fig. 6. White rectangle in the first image is the region shown in the following. Temperature was 380 mK in this case. When the sound pulse was applied from the solid 664 Fizika Nizkikh Temperatur, 2003, v. 29, No. 6 R. Nomura, Y. Suzuki, S. Kimura, Y. Okuda, and S. Burmistrov Fig. 2. Crystallization of 4He induced by sound wave from the solid side. Fig. 3. Melting of 4He crystal induced by sound wave from left to right. Fig. 4. Crystallization of 4He induced by sound wave from left to right. Fig. 5. Crystallization of 4He induced by transverse sound wave from right to left. Manipulation of solid-liquid interface of 4He by acoustic radiation pressure Fizika Nizkikh Temperatur, 2003, v. 29, No. 6 665 Fig. 6. High-speed dynamics of solid-liquid interface trig- gered by sound pulse from the liquid side. White rectangle in the first image is the region shown in the following. Numbers indicate time after the sound pulse in �sec. Fig. 7. High-speed dynamics of solid-liquid interface trig- gered by sound pulse from the solid side. White rectangle in the first image is the region shown in the following. Numbers indicate time after the sound pulse in �sec. side it induced upward motion of the interface first as shown in Fig. 7. These observations demonstrated that interface oscillation or crystallization wave could be excited by the acoustic pulse. When we make a small 4He crystal and apply sound wave to it what will happen? Will it be completely melted or move to the sound direction? It will be very interesting to see if we can move not only the solid-liquid interface but also crystal itself. If this is possible radiation pressure can be used to manipulate 4He crystal in the microgravity. SUMMARY We demonstrated that solid-liquid interface of 4He could be manipulated by sound wave. The interface motion, which was triggered by acoustic radiation pressure, was recorded by using a high-speed CCD camera. It is our future theme to check whether we can manipulate not only the interface but also the crystal itself by acoustic radiation pressure. Acknowledgement This study is partly supported by «Ground-based Research Announcement for Space Utilization» pro- moted by Japan Space Forum. 1. T.G. Wang, E.H. Trinh, A.P. Croonquist, and D.D. Elleman, Phys. Rev. Lett. 56, 452 (1986). 2. R.E. Apfel et al., Phys. Rev. Lett. 78, 1912 (1997). 3. M.J. Marr-Lyon, D.B. Thiessen, and P.L. Marston, Phys. Rev. Lett. 86, 2293 (2001). 4. A.F. Andreev and A.Y. Parshin, Zh. Eksp. Teor. Fiz. 75, 1511 (1978) [Sov. Phys. JETP 48, 763 (1978)]. 5. S. Balibar and P. Noziéres, Solid State Commun. 92, 19 (1994). 6. R. Nomura, M. Maekawa, Y. Suzuki, Y. Okumura, and Y. Okuda, J. Low Temp. Phys. 126, 39 (2002). 7. R. Nomura, Y. Suzuki, S. Kimura, and Y. Okuda, Phys.Rev.Lett. 90, 075301 (2003). 8. M. Sato and T. Fujii, Phys. Rev. E64, 026311 (2001). 666 Fizika Nizkikh Temperatur, 2003, v. 29, No. 6 R. Nomura, Y. Suzuki, S. Kimura, Y. Okuda, and S. Burmistrov