Conical bubble photoluminescence from rhodamine 6G in 1, 2-propanediol

Shou Jie He; Xi Cheng Ai; Li Fang Dong; De Ying Chen; Qi Wang; Xue Chen Li; Jian Ping Zhang; Long Wang

doi:10.1088/1009-1963/15/7/040

Conical bubble photoluminescence from rhodamine 6G in 1, 2-propanediol

Shou Jie He^*
, Xi Cheng Ai
, Li Fang Dong
, De Ying Chen
, Qi Wang
, Xue Chen Li
, Jian Ping Zhang
, Long Wang

^*Corresponding author for this work

School of Astronautics

Hebei University
CAS - Institute of Chemistry
Harbin Institute of Technology
CAS - Institute of Physics

Research output: Contribution to journal › Article › peer-review

8 Scopus citations

Abstract

A modified U-tube conical bubble sonoluminescence device is used to study the conical bubble photoluminescence. The spectra of conical bubble sonoluminescence at different concentrations of rhodamine 6G (Rh6G) solution in 1,2-propanediol have been measured. Results show that the sonoluminescence from the conical bubbles can directly excite Rh6G, which in turn can fluoresce. The light emission of this kind is referred to as conical bubble photoluminescence. The maximum of fluorescence spectral line intensity in the conical bubble photoluminescence has a red shift in relative to that of the standard photo-excited fluorescence, which is due to the higher self-absorption of Rh6G, and the spectral line of conical bubble photoluminescence is broadened in width compared with that of photo-excited fluorescence.

Original language	English
Article number	040
Pages (from-to)	1615-1620
Number of pages	6
Journal	Chinese Physics
Volume	15
Issue number	7
DOIs	https://doi.org/10.1088/1009-1963/15/7/040
State	Published - 1 Jul 2006

Keywords

Cavitation
Conical bubble Photoluminescence
Conical bubble sonoluminescence

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10.1088/1009-1963/15/7/040

Cite this

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title = "Conical bubble photoluminescence from rhodamine 6G in 1, 2-propanediol",

abstract = "A modified U-tube conical bubble sonoluminescence device is used to study the conical bubble photoluminescence. The spectra of conical bubble sonoluminescence at different concentrations of rhodamine 6G (Rh6G) solution in 1,2-propanediol have been measured. Results show that the sonoluminescence from the conical bubbles can directly excite Rh6G, which in turn can fluoresce. The light emission of this kind is referred to as conical bubble photoluminescence. The maximum of fluorescence spectral line intensity in the conical bubble photoluminescence has a red shift in relative to that of the standard photo-excited fluorescence, which is due to the higher self-absorption of Rh6G, and the spectral line of conical bubble photoluminescence is broadened in width compared with that of photo-excited fluorescence.",

keywords = "Cavitation, Conical bubble Photoluminescence, Conical bubble sonoluminescence",

author = "He, \{Shou Jie\} and Ai, \{Xi Cheng\} and Dong, \{Li Fang\} and Chen, \{De Ying\} and Qi Wang and Li, \{Xue Chen\} and Zhang, \{Jian Ping\} and Long Wang",

year = "2006",

month = jul,

day = "1",

doi = "10.1088/1009-1963/15/7/040",

language = "英语",

volume = "15",

pages = "1615--1620",

journal = "Chinese Physics",

issn = "1009-1963",

publisher = "IOP Publishing Ltd.",

number = "7",

}

TY - JOUR

T1 - Conical bubble photoluminescence from rhodamine 6G in 1, 2-propanediol

AU - He, Shou Jie

AU - Ai, Xi Cheng

AU - Dong, Li Fang

AU - Chen, De Ying

AU - Wang, Qi

AU - Li, Xue Chen

AU - Zhang, Jian Ping

AU - Wang, Long

PY - 2006/7/1

Y1 - 2006/7/1

N2 - A modified U-tube conical bubble sonoluminescence device is used to study the conical bubble photoluminescence. The spectra of conical bubble sonoluminescence at different concentrations of rhodamine 6G (Rh6G) solution in 1,2-propanediol have been measured. Results show that the sonoluminescence from the conical bubbles can directly excite Rh6G, which in turn can fluoresce. The light emission of this kind is referred to as conical bubble photoluminescence. The maximum of fluorescence spectral line intensity in the conical bubble photoluminescence has a red shift in relative to that of the standard photo-excited fluorescence, which is due to the higher self-absorption of Rh6G, and the spectral line of conical bubble photoluminescence is broadened in width compared with that of photo-excited fluorescence.

AB - A modified U-tube conical bubble sonoluminescence device is used to study the conical bubble photoluminescence. The spectra of conical bubble sonoluminescence at different concentrations of rhodamine 6G (Rh6G) solution in 1,2-propanediol have been measured. Results show that the sonoluminescence from the conical bubbles can directly excite Rh6G, which in turn can fluoresce. The light emission of this kind is referred to as conical bubble photoluminescence. The maximum of fluorescence spectral line intensity in the conical bubble photoluminescence has a red shift in relative to that of the standard photo-excited fluorescence, which is due to the higher self-absorption of Rh6G, and the spectral line of conical bubble photoluminescence is broadened in width compared with that of photo-excited fluorescence.

KW - Cavitation

KW - Conical bubble Photoluminescence

KW - Conical bubble sonoluminescence

UR - https://www.scopus.com/pages/publications/33745888424

U2 - 10.1088/1009-1963/15/7/040

DO - 10.1088/1009-1963/15/7/040

M3 - 文章

AN - SCOPUS:33745888424

SN - 1009-1963

VL - 15

SP - 1615

EP - 1620

JO - Chinese Physics

JF - Chinese Physics

IS - 7

M1 - 040

ER -

Conical bubble photoluminescence from rhodamine 6G in 1, 2-propanediol

Abstract

Keywords

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