High-precision identification of morphology-dependent resonances in optical processes in microdroplets

J. D. Eversole; H.-B. Lin; A. L. Huston; A. J. Campillo; P. T. Leung; S. Y. Liu; K. Young

doi:10.1364/JOSAB.10.001955

High-precision identification of morphology-dependent resonances in optical processes in microdroplets

J. D. Eversole, H.-B. Lin, A. L. Huston, A. J. Campillo, P. T. Leung, S. Y. Liu, and K. Young

Journal of the Optical Society of America B
Vol. 10,
Issue 10,
pp. 1955-1968
(1993)
•https://doi.org/10.1364/JOSAB.10.001955

Get Citation
Copy Citation Text
J. D. Eversole, H.-B. Lin, A. L. Huston, A. J. Campillo, P. T. Leung, S. Y. Liu, and K. Young, "High-precision identification of morphology-dependent resonances in optical processes in microdroplets," J. Opt. Soc. Am. B 10, 1955-1968 (1993)

Export Citation
- BibTex
- Endnote (RIS)
- HTML
- Plain Text
Get PDF (1443 KB)
Set citation alerts
Save article

Related Topics
Optics & Photonics Topics
?

The topics in this list come from the OSA Optics and Photonics Topics applied to this article.

About this Article
History
- Original Manuscript: December 23, 1992
- Revised Manuscript: April 16, 1993
- Published: October 1, 1993

Not Accessible

Your account may give you access

Abstract

The spectroscopy of the morphology-dependent resonances of a microdroplet has been studied at high precision. The line positions are shown to reveal optical dispersion and permit the refractive index to be determined with sufficient accuracy to provide an estimate of the droplet cooling that is due to evaporation. Comparison of the remaining discrepancies in mode positions for different radial modes indicates a small temperature gradient near the surface. Both the cooling and the temperature gradient are compatible with thermodynamic estimates. The mode quantum numbers are identified with high confidence, and the systematics of the line intensities permit an estimate of the extra radiative loss 1/Q_L over and above that predicted by Lorenz–Mie theory for a perfect homogeneous microsphere, for example, that which is due to internal scattering, with Q_L ≈ 2 × 10⁸ for first-order modes.

Full Article | PDF Article

OSA Recommended Articles

Strong optical force induced by morphology-dependent resonances

Jack Ng, C. T. Chan, Ping Sheng, and Zhifang Lin
Opt. Lett. 30(15) 1956-1958 (2005)

Spectral properties of lasing microdroplets

H-B. Lin, J. D. Eversole, and A. J. Campillo
J. Opt. Soc. Am. B 9(1) 43-50 (1992)

Positions of low-order morphology-dependent resonances determined by elastic light scattering

C. H. Leung, T. C. She, and W. K. Lee
J. Opt. Soc. Am. B 12(7) 1259-1266 (1995)

References

You do not have subscription access to this journal. Citation lists with outbound citation links are available to subscribers only. You may subscribe either as an OSA member, or as an authorized user of your institution.

Contact your librarian or system administrator
or
Login to access OSA Member Subscription

Cited By

You do not have subscription access to this journal. Cited by links are available to subscribers only. You may subscribe either as an OSA member, or as an authorized user of your institution.

Contact your librarian or system administrator
or
Login to access OSA Member Subscription

Figures (11)

You do not have subscription access to this journal. Figure files are available to subscribers only. You may subscribe either as an OSA member, or as an authorized user of your institution.

Contact your librarian or system administrator
or
Login to access OSA Member Subscription

Tables (6)

You do not have subscription access to this journal. Article tables are available to subscribers only. You may subscribe either as an OSA member, or as an authorized user of your institution.

Contact your librarian or system administrator
or
Login to access OSA Member Subscription

Equations (10)

You do not have subscription access to this journal. Equations are available to subscribers only. You may subscribe either as an OSA member, or as an authorized user of your institution.

Contact your librarian or system administrator
or
Login to access OSA Member Subscription

Metrics

You do not have subscription access to this journal. Article level metrics are available to subscribers only. You may subscribe either as an OSA member, or as an authorized user of your institution.

Contact your librarian or system administrator
or
Login to access OSA Member Subscription

No.	Experimental			Theoretical
No.	Position	Height	Width	Position	μ	l	i
1	14 700.8	1.5	3.5	14 697.0	2	76	2
2	14 765.6	0.5	2.8	14 762.1	1	72	3
3	14 782.3	0.6	2.8	–	–	–	–
4	14 865.5	0.5	1.8	14 863.9	2	83	1
5	14 870.8	1.4	3.5	14 868.8	2	77	2
6	14 931.0	0.6	3.5	14 928.3	1	84	1
7	14 941.6	0.4	5.3	14 937.7	1	73	3
8	14 952.2	0.8	3.5	14 949.2	1	78	2
9	15 007.1	0.2	7.1	15 008.7	2	73	3
10	15 030.9	0.6	4.2	15 031.0	2	84	1
11	15 040.8	1.0	5.3	15 040.5	2	78	2
12	15 095.7	0.5	4.2	15 095.3	1	85	1
13	15 113.4	0.4	3.5	15 113.0	1	74	3
14	15 122.2	1.0	3.5	15 120.4	1	79	2
15	15 186.0	0.4	3.5	15 185.0	2	74	3
16	15 196.6	1.5	7.1	15 198.1	2	85	1
17	15 214.3	2.0	4.2	15 212.1	2	79	2
18	15 263.9	1.0	3.5	15 262.2	1	86	1
19	15 292.2	2.0	7.1	15 288.2	1	75	3
				15 291.5	1	80	2
20	15 363.0	1.8	5.3	15 361.1	2	75	3
				15 365.1	2	86	1
21	15 384.3	2.7	3.5	15 383.5	2	80	2
22	15 430.3	1.2	5.3	15 429.0	1	87	1
23	15 464.0	2.8	5.3	15 462.5	1	81	2
23	15 464.0	2.8	5.3	15 463.2	1	76	3
24	15 531.3	2.4	7.1	15 532.0	2	87	1
25	15 540.1	0.5	3.5	15 536.9	2	76	3
26	15 555.2	3.5	3.5	15 554.8	2	81	2
27	15 596.8	1.5	5.3	15 595.8	1	88	1
28	15 634.0	3.0	8.9	15 633.4	1	82	2
29	15 696.8	2.0	5.3	15 698.8	2	88	1
30	15 710.1	1.7	7.1	15 712.6	2	77	3
31	15 726.0	3.7	5.3	15 725.9	2	82	2
32	15 762.3	1.7	5.3	15 762.4	1	89	1
33	15 805.7	3.5	5.3	15 804.2	1	83	2
34	15 813.7	2.0	3.5	15 812.7	1	78	3
35	15 864.2	2.7	7.1	15 865.5	2	89	1
36	15 885.4	2.2	7.1	15 888.0	2	78	3
37	15 896.0	2.2	4.2	15 896.9	2	83	2
38	15 927.9	3.0	5.3	15 929.0	1	90	1
39	15 975.7	5.5	3.5	15 974.8	1	84	2
40	15 986.3	3.0	5.3	15 987.2	1	79	3
41	16 030.6	5.0	4.2	16 032.2	2	90	1
42	16 067.8	9.0	7.1	16 067.8	2	84	2
43	16 096.1	5.0	5.3	16 095.5	1	91	1
44	16 145.7	7.0	5.3	16 145.3	1	85	2
45	16 161.7	4.2	7.1	16 161.5	1	80	3
46	16 197.1	9.0	4.2	16 198.7	2	91	1
47	16 236.9	14.0	4.2	16 238.3	2	80	3
				16 238.6	2	85	2
48	16 260.8	8.0	4.2	16 261.9	1	92	1
49	16 314.8	9.2	4.2	16 315.7	1	86	2
50	16 335.2	6.0	6.4	16 335.6	1	81	3
51	16 363.5	17.0	3.5	16 365.2	2	92	1
52	16 406.9	20.0	5.3	16 409.2	2	86	2
53	16 425.5	11.0	4.2	16 428.3	1	93	1
54	16 483.9	12.0	5.3	16 486.0	1	87	2
55	16 508.7	8.5	5.3	16 509.5	1	82	3
56	16 530.0	53.0	1.8	16 531.6	2	93	1
57	16 577.8	21.0	2.8	16 579.7	2	87	2
58	16 586.6	10.0	1.8	16 587.7	2	82	3
59	16 593.7	15.0	5.3	16 594.6	1	94	1
60	16 655.7	14.5	4.2	16 656.2	1	88	2
61	16 684.0	11.0	5.3	16 683.3	1	83	3
62	16 696.4	Off scale	4.2	16 698.0	2	94	1
63	16 747.8	22.0	1.8	16 750.1	2	88	2
64	16 759.3	29.5	4.2	16 760.8	1	95	1
65	16 825.7	17.0	4.2	16 826.2	1	89	2
66	16 857.5	14.0	1.8	16 857.0	1	84	3
67	16 862.9	Off scale	3.5	16 864.2	2	95	1
68	16 919.5	30.0	1.8	16 920.4	2	89	2
69	16 926.6	34.0	3.5	16 926.9	1	96	1
70	16 935.5	21.0	3.5	16 936.4	2	84	3
71	16 995.7	21.0	5.3	16 996.2	1	90	2
72	17 029.3	Off scale	2.8	17 030.4	2	96	1
				17 030.5	1	85	3
73	17 091.3	Off scale	3.5	17 090.6	2	90	2
				17 093.0	1	97	1
74	17 109.0	23.0	4.2	17 110.5	2	85	3
75	17 165.7	25.0	6.4	17 166.0	1	91	2
76	17 195.8	56.0	2.8	17 196.5	2	97	1
77	17 204.6	21.0	6.4	17 203.8	1	86	3
78	17 259.5	Off scale	3.5	17 258.9	1	98	1
				17 260.6	2	91	2
79	17 284.3	29.0	3.5	17 284.4	2	86	3
80	17 300.2	2.0	12.4	17 298.2	1	82	4
81	17 335.6	30.0	5.3	17 335.8	1	92	2
82	17 360.4	27.0	3.5	17 362.6	2	98	1
83	17 377.3	24.0	7.1	17 377.0	1	87	3
84	17 413.2	19.0	1.8	–	–	–	–
85	17 431.2	50.0	3.5	17 430.5	2	92	2
86	17 457.8	30.0	5.3	17 458.1	2	87	3
87	17 477.3	3.0	15.9	17 474.7	1	83	4
88	17 505.6	32.0	4.2	17 505.4	1	93	2
89	17 528.7	18.0	3.5	17 528.5	2	99	1
				17 531.8	2	83	4
90	17 551.7	33.0	6.4	17 550.0	1	88	3
91	17 588.8	6.0	3.5	17 590.7	1	100	1
92	17 599.5	48.0	2.8	17 600.4	2	93	2
93	17 631.3	50.0	3.5	17 631.6	2	88	3
94	17 652.5	5.0	15.9	17 651.0	1	84	4
95	17 675.6	22.0	5.3	17 674.9	1	94	2
96	17 693.3	4.0	5.3	17 694.4	2	100	1
97	17 709.3	2.0	8.9	17 709.3	2	84	4
98	17 725.2	36.0	5.3	17 722.9	1	89	3
99	17 757.1	2.0	7.1	17 756.5	1	101	1
100	17 771.2	30.0	2.1	17 770.1	2	94	2
101	17 804.9	53.0	3.5	17 805.0	2	89	3
102	17 829.7	4.0	8.9	17 827.1	1	85	4
103	17 845.6	8.0	5.3	17 844.4	1	95	2
104	17 859.8	2.0	5.3	17 860.3	2	101	1
105	17 882.8	3.0	3.5	17 886.6	2	85	4
106	17 897.0	37.0	4.2	17 895.6	1	90	3
107	17 939.5	11.0	3.5	17 939.7	2	95	2
108	17 978.4	47.0	3.5	17 978.2	2	90	3
109	18 006.7	6.0	10.6	18 003.1	1	86	4
110	18 015.6	3.0	3.5	18 013.7	1	96	2
111	18 070.5	29.0	6.4	18 068.2	1	91	3
112	18 109.4	2.0	2.1	18 109.2	2	96	2
113	18 151.9	26.0	3.5	18 151.3	2	91	3
114	18 183.8	4.0	10.6	18 182.9	1	97	2
115	18 242.3	11.0	6.4	18 240.6	1	92	3
				18 240.7	2	87	4
116	18 325.5	4.5	5.3	18 324.2	2	92	3
117	18 355.6	1.0	10.6	18 352.1	1	98	2
				18 354.7	1	88	4
118	18 414.0	1.0	3.5	18 413.0	1	93	3
				18 417.5	2	88	4

Experimental		Theoretical
No.	Position	Position	μ	l	i
1	16 141.7	16 141.9	2	86	3
2	16 191.6	16 191.0	1	92	2
3	16 214.1	16 215.9	2	98	1
4	16 230.0	16 229.1	1	87	3
5	16 274.0	16 274.4	1	99	1
6	16 279.3	16 279.0	2	92	2
7	16 304.3	16 304.2	2	87	3
8	16 350.1	16 349.4	1	93	2
9	16 369.9	16 370.9	2	99	1
		16 372.2	2	83	4
10	16 392.6	16 390.7	1	88	3
11	16 428.9	16 429.2	1	100	1
12	16 437.8	16 437.6	2	93	2
13	16 466.5	16 466.3	2	88	3
14	16 508.3	16 507.7	1	94	2
15	16 524.7	16 525.8	2	100	1
16	16 553.5	16 552.2	1	89	3
17	16 583.3	16 584.0	1	101	1
18	16 596.3	16 596.1	2	94	2
19	16 628.4	16 628.2	2	89	3
20	16 650.8	16 649.0	1	85	4
21	16 666.4	16 665.9	1	95	2
22	16 678.8	16 680.6	2	101	1
23	16 714.7	16 713.5	1	90	3
24	16 737.5	16 738.7	1	102	1
25	16 754.3	16 754.5	2	95	2
26	16 790.2	16 789.9	2	90	3
27	16 824.8	16 824.1	1	96	2
28	16 834.2	16 835.4	2	102	1
29	16 875.8	16 874.7	1	91	3
30	16 892.4	16 893.4	1	103	1
31	16 912.6	16 912.8	2	96	2
32	16 952.0	16 951.6	2	91	3
33	16 982.5	16 982.1	1	97	2
34	16 988.7	16 990.1	2	103	1
35	17 036.8	17 034.1	2	87	4
		17 035.7	1	92	3
36	17 046.9	17 048.0	1	104	1
37	17 070.8	17 070.9	2	97	2
38	17 113.4	17 113.0	2	92	3
		17 140.0	1	98	2
39	17 141.0	17 141.7	1	88	4
		17 144.7	2	104	1
		17 140.0	1	98	2
40.	17 143.1	17 141.7	1	88	4
		17 144.7	2	104	1
41	17 198.0	17 196.6	1	93	3
		17 199.2	2	88	4
42	17 201.5	17 199.2	2	88	4
		17 202.5	1	105	1
43	17 228.6	17 229.0	2	98	2
44	17 274.5	17 274.4	2	93	3
45	17 298.2	17 297.8	1	99	2
		17 299.3	2	105	1
46	17 357.9	17 357.0	1	106	1
		17 357.4	1	94	3
47	17 386.8	17 387.0	2	99	2
48	17 435.5	17 435.6	2	94	3
49	17 455.3	17 453.8	2	106	1
		17 455.6	1	100	2
50	17 470.2	17 469.3	1	90	4
51	17 510.8	17 511.4	1	107	1
52	17 518.6	17 518.1	1	95	3
53	17 529.4	17 528.8	2	90	4
54	17 544.8	17 544.9	2	100	2
55	17 596.8	17 596.6	2	95	3
56	17 607.1	17 608.2	2	107	1
57	17 613.7	17 613.2	1	101	2
58	17 633.9	17 632.9	1	91	4
59	17 664.9	17 665.7	1	108	1
60	17 679.7	17 678.6	1	96	3
61	17 692.6	17 693.3	2	91	4
62	17 702.0	17 702.7	2	101	2
63	17 757.5	17 757.5	2	96	3
64	17 771.0	17 770.8	1	102	2
65	17 797.3	17 796.4	1	92	4
66	17 818.4	17 820.0	1	109	1
67	17 839.6	17 839.1	1	97	3
68	17 859.4	17 857.7	2	92	4
		17 860.4	2	102	2
69	17 918.5	17 916.9	2	109	1
		17 918.3	2	97	3
70	17 960.6	17 959.7	1	93	4
71	18 000.1	17 999.4	1	98	3
72	18 019.6	18 018.0	2	103	2
		18 021.9	2	93	4
73	18 079.1	18 079.0	2	98	3
74	18 124.1	18 122.8	1	94	4
75	18 160.3	18 159.6	1	99	3
76	18 185.1	18 185.8	2	94	4
77	18 239.7	18 239.5	2	99	3
		18 243.0	1	105	2
78	18 286.7	18 285.8	1	95	4
79	18 320.3	18 319.7	1	100	3
80	18 349.6	18 349.6	2	95	4
81	18 399.8	18 399.9	2	100	3
		18 400.2	1	106	2
82	18 449.4	18 448.7	1	96	4
83	18 480.0	18 479.7	1	101	3
84	18 512.9	18 513.3	2	96	4
85	18 559.7	18 557.3	1	107	2
		18 560.2	2	101	3
86	18 611.9	18 611.4	1	97	4
87	18 640.1	18 639.5	1	102	3
88	18 676.3	18 676.7	2	97	4
89	18 719.9	18 720.3	2	102	3
90	18 774.3	18 774.0	1	98	4
91	18 799.7	18 799.3	1	103	3
92	18 839.0	18 840.0	2	98	4
		18 841.4	2	115	1
93	18 879.0	18 880.4	2	103	3
94	18 936.0	18 936.4	1	99	4

Data Set	n	a (μm)	C	S	l^*
A	1.348	7.301	0.792	110 (93%)	97
B	1.347	7.897	0.722	72 (77%)	–

Data Set	n	a (μm)	Δx	C	S	l^*
A	1.364	7.226	0.85	0.909	117 (99%)	96
B	1.364	7.763	1.12	0.954	94 (100%)	–

Data Set	n₀	n₁(10⁻⁶ cm)	a (μm)	C	S	l^*
A	1.366	0.964	7.133	0.883	116 (98%)	96
B	1.365	1.06	7.652	0.962	94 (100%)	–

Polarization	Mode Order i
Polarization	1	2	3
TE	4 × 10⁻⁷	5 × 10⁻⁶	<10⁻⁴
TM	4 × 10⁻⁷	4 × 10⁻⁶	<10⁻⁴

Abstract

References

Cited By

Figures (11)

Tables (6)

Equations (10)

Metrics

Login or Create Account