• 検索結果がありません。

mea-sured for an ensemble. We derived the radiative and non-radiative decay rates for single q-dots from the fluorescence quantum efficiency and total decay rate of its ex-cited state. We demonstrated that fluorescence quantum efficiency of single q-dots degraded in time. This degradation in the fluorescence quantum efficiency of single q-dots may limit the applications in quantum information science. In order to pre-vent such degradation, one possible idea is to coat the nanofiber with a polymer after depositing the q-dots.

We have experientally investigated the effect of q-dot azimuthal position on the estimation of the channeling efficiency for various fiber diameters, especially thicker fiber diameters.

7.2. Future Prospects 73

FBG

High quantum efficiency q-dot

Figure 7.1: Schematic diagram of the experimental setup. A high quantum efficiency q-dot is deposited in the nanofiber cavity. FBG denotes fiber Bragg grating.

However, when we combine a q-dot with a nanofiber cavity, a narrow emission spectrum would be necessary in order to realize enhancement. As we demonstrated in Chapter 3, one can readily measure emission spectrum of single q-dots using a nanofiber technique. In the experiments performed so far, we excited the q-dot well above the band edge (excitation wavelength=640 nm, emission wavelength=800 nm).

The measured spectrum width was about 52 nm. The mechanism of the broadening may be understood to be due to spectral diffusion and exciton-phonon interactions.

In order to get narrow linewidth, one promising way is to excite the q-dot at its band edge. This kind of approach should be investigated systematically. Furthermore, a nanofiber-cavity system combined with advanced quantum emitters, such as un-blinking color centers in nanodiamonds [95, 96], may provide a new route to achieve on-demand single-photon generation into single-mode optical fibers.

[1] J. I. Cirac, P. Zoller, H. J. Kimble, and H. Mabuchi, “Quantum State Transfer and Entanglement Distribution among Distant Nodes in a Quantum Network,”

Phys. Rev. Lett., 78, 3221 (1997).

[2] H. J. Kimble, “The quantum internet,” Nature453, 1023-1030 (2008).

[3] S. Ritter, C. Nolleke, C. Hahn, A. Reiserer, A. Neuzner, M. Uphoff, M. Mucke, E. Figueroa, J. Bochmann, and G. Rempe, “An elementary quantum network of single atoms in optical cavities,” Nature 484, 195-199 (2012).

[4] S. -B. Zheng and G. -C. Guo, “Efficient Scheme for Two-Atom Entanglement and Quantum Information Processing in Cavity QED,” Phys. Rev. Lett. 85, 2392 (2000).

[5] O. Benson, C. Santori, M. Pelton, and Y. Yamamoto, “Regulated and entangled photons from a single quantum dot,” Phys. Rev. Lett. 84, 2513 (2000).

[6] H. J. Kimble, M. Dagenais, and L. Mandel, “Photon antibunching in resonance fluorescence,” Phys. Rev. Lett., 39, 691 (1977).

[7] R. J. Thompson, G. Rempe, and H. J. Kimble, “Observation of normal-mode splitting for an atom in an optical cavity,” Phys. Rev. Lett., 68, 1132 (1992).

75

References 76

[8] C. J. Hood, M. S. Chapman, T. W. Lynn, and H. J. Kimble, “Real-time cavity QED with single atoms,” Phys. Rev. Lett., 80, 4157 (1998).

[9] J. Ye, D. W. Vernooy, and H. J. Kimble, “Trapping of single atoms in cavity QED,” Phys. Rev. Lett. 83, 4987 (1999).

[10] C. J. Hood, T. W. Lynn, A. C. Doherty, A. S. Parkins and H. J. Kimble, “The atom-cavity microscope: single atoms bound in orbit by single photons,” Science, 287, 1447 (2000).

[11] P. W. H. Pinkse, T. Fischer, P. Maunz, and G. Rempe, “Trapping an atom with single photons,” Nature 404, 365 (2000).

[12] F. Diedrich and H. Walther, “Nonclassical radiation of a single stored ion,” Phys.

Rev. Lett. 58, 203 (1987).

[13] Th. Basche and W. E. Moerner, “Photon antibunching in the fluorescence of a single dye molecule trapped in a solid,” Phys. Rev. Lett. 69, 1516 (1992).

[14] F. D. Martini, G. D. Giuseppe, and M. Marracco, “Single-mode generation of quantum photon states by excited single molecules in a microcavity trap,” Phys.

Rev. Lett. 76, 900 (1996).

[15] C. Brunel, B. Lounis, P. Tamarat, and M. Orrit, “Triggered source of single photons based on controlled single molecule fluorescence,” Phys. Rev. Lett. 83, 2722 (1999).

[16] L. Fleury, J. -M. Segura, G. Zumofen, B. Hecht, and U. P. Wild, “Nonclassical photon statistics in single-molecule fluorescence at room temperature,” Phys.

Rev. Lett. 84, 1148 (2000).

[17] B. Lounis and W. E. Moerner, “Single photons on demand from a single molecule at room temperature,” Nature (London) 407, 491 (2000).

[18] C. Kurtsiefer, S. Mayer, P. Zarda, and H. Weinfurter, “Stable Solid-State Source of Single Photons,” Phys. Rev. Lett. 85, 290-293 (2000).

[19] R. Brouri, A. Beveratos, J. -P. Poizat, and P. Grangier, “Photon antibunching in the fluorescence of individual color centers in diamond,” Opt. Lett. 25, 1294 (2000).

[20] A. Beveratos, S. Kuehn, R. Brouri, T. Gacoin, J. -P. Poizat, and P. Grang-ier, “Room temperature stable single-photon source,” Eur. Phys. J. D, 18, 191 (2002).

[21] J. Kim, O. Benson, H. Kan, and Y. Yamamoto, “A single-photon turnstile de-vice,” Nature (London) 397, 500 (1999).

[22] P. Michler, A. Imamoglu, M. D. Mason, P. J. Carson, G. F. Strouse, and S. K.

Buratto, “Quantum correlation among photons from a single quantum dot at room temperature,” Nature 406, 968 (2000).

[23] B. Lounis, H. A. Bechtel, D. Gerion, P. Alivisatos, and W. E. Moerner, “Photon antibunching in single CdSe/ZnS quantum dot fluorescence,” Chem. Phys. Lett.

329, 399-404 (2000).

[24] P. Michler, A. Kiraz, C. Becher, W. V. Schoenfeld, P. M. Petro, L. Zhang, E.

Hu, and A. Imamoglu, “A quantum dot single-photon turnstile device,” Science 290, 2282 (2000).

[25] C. Santori, M. Pelton, G. Solomon, Y. Dale, and Y. Yamamoto, “Triggered single photons from a quantum dot,” Phys. Rev. Lett. 86, 1502 (2001).

[26] V. Zwiller, H. Blom, P. Jonsson, N. Panev, S. Jeppesen, T. Tsegaye, E. Goobar, M.-E. Pistol, L. Samuelson, and G. Bjork, “Single quantum dots emit single photons at a time: antibunching experiments,” Appl. Phy. Lett.78, 2476 (2001).

[27] E. Moreau, I. Robert, J. -M. Gerard, I. Abram, L. Manin, and V. Thierry-Mieg,

“Single-mode solid-state single photon source based on isolated quantum dots in pillar microcavities,” App. Phy. Lett. 79, 2865 (2001).

References 78

[28] R. M. Thompson, R. M. Stevenson, A. J. Shields, I. Farrer, C. J. Lobo, D. A.

Ritchie, M. L. Leadbeater, and M. Pepper, “Single-photon emission from exciton complexes in individual quantum dots,” Phy. Rev. B 64, 201302-1 (2001).

[29] G. Solomon, M. Pelton, and Y. Yamamoto, “Single-mode Spontaneous Emission from a Single Quantum Dot in a Three-Dimensional Microcavity,” Phys. Rev.

Lett. 86, 3903 (2001).

[30] M. Pelton, C. Santori, J. Vuckovic, B. Zhang, G. S. Solomon, J. Plant, and Y.

Yamamoto, “Efficient Source of Single Photons: A Single Quantum Dot in a Micropost Microcavity,” Phys. Rev. Lett. 89, 233602 (2002).

[31] C. Santori, D. Fattal, J. Vuckovic, G. S. Solomon, and Y. Yamamoto, “Indis-tinguishable Photons from a Single-Photon Device,” Nature (London) 419, 594 (2002).

[32] Z. Yuan, B. E. Kardynal, R. M. Stevenson, A. J. Shields, C. J. Lobo, K. Cooper, N. S. Beattie, D. A. Ritchie, and M. Pepper, “Electrically driven single photon source,” Science295, 102 (2002).

[33] K. Vahala, “Optical microcavities,” Nature 424, 839-846 (2003).

[34] A. V. Akimov, A. Mukherjee, C. L. Yu, D. E. Chang, A. S. Zibrov, P. R. Hemmer, H. Park, and M. D. Lukin, “Generation of single optical plasmons in metallic nanowires coupled to quantum dots,” Nature 450, 402-406 (2007).

[35] G. Shambat, J. Provine, K. Rivoire, T. Sarmiento, J. Harris, and J. Vuckovic,

“Optical fiber tips functionalized with semiconductor photonic crystal cavities,”

Appl. Phys. Lett. 99, 191102 (2011).

[36] T. Schroder, A. W. Schell, G. Kewes, T. Aichele, and O. Benson, “Fiber-Integrated Diamond-Based Single Photon Source,” Nano Lett. 11, 198-202 (2010).

[37] T. Schroder, F. Gadeke, M. J. Banholzer, and O. Benson, “Ultrabright and efficient single-photon generation based on nitrogen-vacancy centres in nanodia-monds on a solid immersion lens,” New J. Phys.13, 055017 (2011).

[38] F. Haupt, S. S. R. Oemrawsingh, S. M. Thon, H. Kim, D. Kleckner, D. Ding, D.

J. Suntrup, P. M. Petroff, and D. Bouwmeester, “Fiber-connectrized micropillar cavities” Appl. Phys. Lett. 97, 131113 (2010).

[39] V. V. Klimov and M. Ducloy, “Spontaneous emission rate of an excited atom placed near a nanofiber,” Phys. Rev. A 69, 013812 (2004).

[40] F. L. Kien, S. Dutta Gupta, V. I. Balykin, and K. Hakuta, “Spontaneous emission of a cesium atom near a nanofiber: Efficient coupling of light to guided modes,”

Phys. Rev. A 72, 032509 (2005).

[41] K. P. Nayak, P. N. Melentiev, M. Morinaga, Fam Le Kien, V. I. Balykin, and K. Hakuta, “Optical nanofiber as an efficient tool for manipulating and probing atomic fluorescence,” Opt. Express 15, 5431 (2007).

[42] A. Stiebeiner, R. Garcia-Fernandez, and A. Rauschenbeutel, “Design and op-timization of broadband tapered optical fibers with a nanofiber waist,” Opt.

Express 18, 22677-22685 (2010).

[43] A. K. Patnaik, J. Q. Liang, and K. Hakuta “Slow light propagation in a thin optical fiber via electromagnetically induced transparency,” Phys. Rev. A 66, 063808 (2002).

[44] L. Tong, R. R. Gattass, J. B. Ashcom, S. He, J. Lou, M. Shen, I. Maxwell, and E.

Mazur, “Subwavelength-diameter silica wires for low-loss optical wave guiding,”

Nature (London) 426, 816 (2003).

[45] T. A. Birks, W. J. Wadsworth, and P. St. J. Russell, “Supercontinuum generation in tapered fibers,” Opt. Lett. 25, 1415 (2000).

References 80

[46] M. Cai, O. Painter, and K. J. Vahala, “Observation of critical coupling in a fiber taper to a silica-microsphere whispering-gallery mode system,” Phys. Rev. Lett.

85, 74 (2000).

[47] F. L. Kien, J. Q. Liang, K. Hakuta, and V. I. Balykin, “Field intensity distri-butions and polarization orientations in a vacuum-clad subwavelength-diameter optical fiber,” Opt. Comm. 242, 445 (2004).

[48] E. M. Purcell, “Spontaneous emission probabilities at radio frequencies,” Phys.

Rev. 69, 681 (1946).

[49] K. P. Nayak and K. Hakuta, “Single atoms on an optical nanofiber,” New J.

Phys. 10, 053003 (2008).

[50] K. P. Nayak, Fam Le Kien, M. Morinaga, and K. Hakuta, “Antibunching and bunching of photons in resonance fluorescence from a few atoms into guided modes of an optical nanofiber,” Phys. Rev. A 79, 021801(R) (2009).

[51] K. P. Nayak, Thesis, Department of Applied Physics and Chemistry, University of Electro-Communications, Japan.

[52] M. Das, A. Shirasaki, K. P. Nayak, M. Morinaga, F. L. Kien, and K. Hakuta,

“Measurement of fluorescence emission spectrum of few strongly driven atoms using an optical nanofiber,” Opt. Express 18, 17154-17164 (2010).

[53] Manoj Das, Thesis, Department of Applied Physics and Chemistry, University of Electro-Communications, Japan.

[54] V. I. Balykin, K. Hakuta, Fam Le Kien, J. Q. Liang, and M. Morinaga, “Atom trapping and guiding with a subwavelength-diameter optical fiber,” Phys. Rev.

A, 70, 011401(R) (2004).

[55] F. L. Kien, V. I. Balykin, and K. Hakuta, “Atom trap and waveguide using a two-color evanescent light field around a subwavelength-diameter optical fiber,”

Phys. Rev. A 70, 063403 (2004).

[56] G. Sague, A. Baade, and A. Rauschenbeutel, “Blue-detuned evanescent field surface traps for neutral atoms based on mode interference in ultra-thin optical fibres,” New J. Phys. 10, 113008 (2008).

[57] E. Vetsch, D. Reitz, G. Sague, R. Schmidt, S. T. Dawkins, and A. Rauschenbeu-tel, “Optical interface created by laser-cooled atoms trapped in the evanescent field surrounding an optical nanofiber,” Phys. Rev. Lett. 104, 203603 (2010).

[58] A. Goban, K. S. Choi, D. J. Alton, D. Ding, C. Lacroute, M. Pototschnig, T.

Thiele, N. P. Stern, and H. J. Kimble, “Demonstration of a State-Insensitive, Compensated Nanofiber Trap,” Phys. Rev. Lett. 109, 033603 (2012).

[59] J. M. Ward, D. G. OShea, B. J. Shortt, M. J. Morrissey, K. Deasy, and S.G. Nic Chormaic, “Heat-and-pull rig for fiber taper fabrication,” Rev. Sci. Instrum.77, 083105 (2006).

[60] J. D. Love, W. M. Henry, W. J. Stewart, R. J. Black, S. Lacroix, and F. Gonthier,

“Tapered single-mode fibers and devices,” IEE Proc.-J: Optoelectron. 138, 343 (1991).

[61] T. A. Birks and Y. W. Li, “The shape of fiber tapers,” J. Lightwave Tech. 10, 432 (1992).

[62] M. Sumetsky, “How thin can a microfiber be and still guide light?,” Opt. Lett.

31, 870 (2006).

[63] T. E. Dimmick, G. Kakarantzas, T. A. Birks, and P. St. J. Russell, “Carbon dioxide laser fabrication of fused-fiber couplers and tapers,” Appl. Opt.38, 6845 (1999).

[64] M. Sumetsky, Y. Dulashko, and A. Hale, “Fabrication and study of bent and coiled free silica nanowires: Self-coupling microloop optical interferometer,” Opt.

Express 12, 3521 (2004).

References 82

[65] Y. Takeuchi and J. Noda, “Novel Fiber Coupler Tapering Process Using a Mi-croheater,” IEEE Photonics Tech. Lett.4, 465, (1992).

[66] Y. Takeuchi, M. Hirayama, S. Sumida, and O. Kobayashi, “Characteristics of ceramic microheater for fiber coupler fabrication,” Jpn. J. Appl. Phys. 37, 3665 (1998).

[67] Quantum Dots, “Qdot ITK Carboxyl Quantum Dots user manual”.

[68] Subpicoliter needle dispenser, “Applied Micro Systems, ND-2000 user manual”.

[69] Inverted Microscope,“ Nikon Eclipse Ti-U user manual (M449E3)”.

[70] High precision X-Y stage, “BIOS-T Series user manual (BIOS 305-T)”.

[71] R. Hanbury Brown and R. Q. Twiss, “Correlation between Photons in two Co-herent Beams of Light,” Nature (London) 177, 27 (1956).

[72] Invitrogen, Certificate of analysis Q21371MP, Lot Number:834674. In the com-pany quotation, the quantum efficiency was measured relatively to rhodamine 101 by assuming the quantum efficiency of rhodamine 101 to be 100%.

[73] T. Karstens and K. Kobs, “Rhodamine B and rhodamine 101 as reference sub-stances for fluorescence quantum yield measurements,” J. Phys. Chem.84, 1871-1872 (1980).

[74] M. Nirmal, B. O. Dabbousi, M. G. Bawendi, J. J. Macklin, J. K. Trautman, T. D. Harris, and L. E. Brus, “Fluorescence intermittency in single cadmium selenide nanocrystals,” Nature 383, 802-804 (1996).

[75] Al. L. Efros and M. Rosen, “Random telegraph signal in the photoluminescence intensity of a single quantum dot,” Phys. Rev. Lett. 78, 1110-1113 (1997).

[76] M. Kuno, D. P. Fromm, H. F. Hamann, A. Gallagher, and D. J. Nesbitt, “Non-exponential “blinking” kinetics of single CdSe quantum dots:A universal power law behavior,” J. Chem. Phys. 112, 3117-3120 (2000).

[77] M. Kuno, D. P. Fromm, H. F. Hamann, A. Gallagher, and D. J. Nesbitt,

““On”/“off” fluorescence intermittency of single semiconductor quantum dots,”

J. Chem. Phys. 115, 1028-1040 (2001).

[78] R. Loudon, Quantum Theory of Light (Oxford University Press, Oxford, 2000).

[79] S. A. Empedocles, R. Neuhauser, K. Shimizu, and M. G. Bawendi, “Photolumi-nescence from single semiconductor nanostructures,” Adv. Mater.11, 1243-1256 (1999).

[80] R. Arians, T. Kummell, G. Bacher, A. Gust, C. Kruse, and D. Hommel, “Room temperature emission from CdSe/ZnSSe/MgS single quantum dots,” Appl. Phys.

Lett. 90, 101114 (2007).

[81] K. Goushi, T. Yamada, and A. Otomo, “Excitation Intensity Dependence of Power-Law Blinking Statistics in Nanocrystal Quantum Dots,” J. Phys. Chem.

C 113, 20161 (2009).

[82] Ramachandrarao Yalla, K. P. Nayak, and K. Hakuta, “Fluorescence photon mea-surements from single quantum dots on an optical nanofiber,” arXiv:1112.0624v1 (2011).

[83] Ramachandrarao Yalla, K. P. Nayak, and K. Hakuta, “Fluorescence photon mea-surements from single quantum dots on an optical nanofiber,” Opt. Express 20, 2932-2941 (2012).

[84] T. Ota, K. Maehashi, H. Nakashima, K. Oto, and K. Murase,“Photodegradation of CdSe Quantum Dots Studied by Micro-Photoluminescence Spectroscopy,”

Phys. Status Solidi B 224, 169 (2001).

[85] Wolfgang Alt, “An objective lens for efficient fluorescence detection of single atoms,” Optik 113, 142-144 (2002).

[86] J. A. Stratton, ElectromagneticTheory (McGraw-Hill, New York, 1941), Chap.

6; Details will be reported elsewhere.

References 84

[87] B. R. Fisher, H. J. Eisler, N. E. Stott, and M. G. Bawendi, “Emission Intensity Dependence and Single-Exponential Behavior In Single Colloidal Quantum Dot Fluorescence Lifetimes,” J. Phys. Chem. B 108, 143 (2004).

[88] Invitrogen, Certificate of analysis Q21371MP, Lot Number: 898274. In the com-pany quotation, the quantum efficiency was measured relatively to rhodamine 101 by assuming the quantum efficiency of rhodamine 101 to be 100%.

[89] S. V. Kershaw, M. Burt, M. Harrison, A. Rogach, H. Weller, and A. Eychmuller,

“Colloidal CdTe/HgTe quantum dots with high photoluminescence quantum ef-ficiency at room temperature,” Appl. Phys. Lett. 75, 1694 (1999).

[90] X. Brokmann, L. Coolen, M. Dahan, and J. P. Hermier, “Measurement of the Radiative and Nonradiative Decay Rates of Single CdSe Nanocrystals through a Controlled Modification of their Spontaneous Emission,” Phys. Rev. Lett. 93, 107403 (2004).

[91] M. Grabolle, M. Spieles, V. Lesnyak, N. Gaponik, A. Eychmuller, and U. Resch-Genger, “Determination of the Fluorescence Quantum Yield of Quantum Dots:

Suitable Procedures and Achievable Uncertainties,”Anal. Chem. 81, 6285-6294 (2009).

[92] Ramachandrarao Yalla, Fam Le Kien, M. Morinaga, and K. Hakuta, “Efficient channeling of fluorescence photons from single quantum dots into guided modes of optical nanofiber,” Phys. Rev. Lett. 109, 063602 (2012).

[93] F. L. Kien and K. Hakuta, “Cavity-enhanced channeling of emission from an atom into a nanofiber,” Phys. Rev. A80, 053826 (2009).

[94] K. P. Nayak, F. L. Kien, Y. Kawai, K. Hakuta, K. Nakajima, H. T. Miyazaki, and Y. Sugimoto, “Cavity formation on an optical nanofiber using focused ion beam milling technique,” Opt. Express 19, 14040-14050 (2011).

[95] I. Aharonovich, S. Castelletto, D. A. Simpson, C-H. Su, A. D. Greentree, and S. Prawer,“Diamond-based single-photon emitters,” Rep. Prog. Phys.74 076501 (2011).

[96] E. Neu, D. Steinmetz, J. Riedrich-Moller, S. Gsell, M. Fischer, M. Schreck, and C.

Becher, “Single photon emission from silicon-vacancy colour centres in chemical vapour deposition nano-diamonds on iridium,” New J. Phys. 13 025012 (2011).

[97] W. G. J. H. M. van Sark, P. L. T. M. Frederix, A. A. Bol, H. C. Gerritsen, and A. Meijerink, “Blueing, Bleaching, and Blinking of Single CdSe/ZnS Quantum Dots,” Chem. Phys. Chem., 3, 871-879 (2002).

Appendix A

Degradation of Single Quantum Dots

0 10 20 30

Time [s]

0 100 200 300 400

Ph ot on c ou nt r at e [k cp s]

Figure A.1: Typical fluorescence photon-count rate as a function of time before degra-dation of the q-dot.

Figure A.1 shows a typical measurement of the fluorescence photon-count rate as a function of time before the single q-dot degraded. In order to protect the q-dot from oxidation, we flow nitrogen gas continuously for the whole experiment period.

However, the sudden drop in the fluorescence count might be explained by the forma-87

tion of lattice defects, which creates additional non-radiative recombination pathways (permanent quenching states). Due to photoinduced quenching states, at a high laser power q-dot degradation is expected [97].

Appendix B

Certificate of Analysis

For the experiments in this thesis, we use a carboxyl colloidal CdSeTe/ZnS q-dots [72, 88]. The followings are Certificate of Analysis (CoA) provided by the Invitrogen company.

B.1 CoA for Lot Number: 834674

Catalog Number: Q21371MP

Product Name: Qdot 800 ITK carboxyl quantum dots “8 µM solution”

Appearance: black suspension

Medium: 50 mM borate buffer, pH 9.0 Lot Number: 834674

89

LOT DATA SPECIFICATION ABSORBANCE

Concentration 7.9 µM 7.5-8.5 µM

FLUORESCENCE

Emission Maximum 792 nm 795 (±10) nm

Relative Quantum Yield1 72% ≥35%

Full Width at Half Maximum 82 nm ≤100 nm

1. Quantum yield determined relative to rhodamine 101.

B.2 CoA for Lot Number: 898274

Catalog Number: Q21371MP

Product Name: Qdot 800 ITK carboxyl quantum dots “8 µM solution”

Appearance: black suspension

Medium: 50 mM borate buffer, pH 9.0 Lot Number: 898274

LOT DATA SPECIFICATION

ABSORBANCE

Concentration 8.4 µM 7.5-8.5 µM

FLUORESCENCE

Emission Maximum 797 nm 795 (±10) nm

Relative Quantum Yield1 56% ≥35%

Full Width at Half Maximum 66 nm ≤100 nm

1. Quantum yield determined relative to rhodamine 101.

Acknowledgements

I would like to express my sincere thanks to many people for their continuous support during my journey of research in the last four years. First and foremost, I would like to sincerely thank to my Ph.D supervisor Professor Kohzo Hakuta (Hakuta sensei) for his valuable guidance and giving me interesting projects to work on with constant encouragement in his Laboratory. Hakuta sensei trained me in all possible direc-tions in the research with his experience, knowledge and talent. For example, logical thinking, writing scientific articles and presenting skills. I should mention here that, inspite of his very busy schedule, we are always welcome in his room to discuss re-search problem, without any prior appointments. As if now, I have learned so much of knowledge and experience by working in his Laboratory and discussing with sensei.

I hope that my hunger for learning ever last.

Here, I would like to express my thanks to my laboratory seniors and colleagues, who helped me in the experiments during my work. Here the first person comes in line, I would like to sincerely thank to my super senior Dr. Kali Prasanna Nayak, who helped me during my entire research period. I am very fortunate enough that his stay in our laboratory overlapped with mine. During Kali stay in the Laboratory, I have learned many experimental technique, mainly how to fix the problem. I would like to sincerely thank to Prof. Fam Le Kien, who helped me the theoretical part under-standing of our nanofiber experiments. I would like to sincerely thank to Morinaga Sensei of Institute of Laser Science in our University to teach me various experimen-tal details and software skills. Here, I should mention that I used Morinaga sensei C program entire my thesis. I would like to sincerely thank my senior Dr. Manoj Das, who helped me not only in the experimental room but also in general life in Japan. I would like to sincerely thank to Dr. Mark Sadgrove for his help during final days of my thesis writing. I would like to thank my laboratory members Oyamoto, Oyama, Yuto, Kojima, Yamashita, Sakaguchi and Yazawa.

I would like to express my sincere thank to the members of review committee for my Ph.D. work. I would like to thank Prof. Kohzo Hakuta, Prof. Kouichi Yamaguchi,

san. I am indebted to my Japanese language teachers Ikeda sensei, Tanaka sensei, Miyoshi sensei and Ooki sensei who taught me the basic Japanese languages and introduce me to the Japanese culture. I am also grateful to my other Japanese language teacher Oohori Sensei, who taught me Japanese language in a local volunteer society.

I would also like to acknowledge my friends here, Raju, Manasa, Maruthi Manoj, Srinu, Sanjay, Rakesh, Jameesh and Vikram.

Finally, this thesis would not have been possible without the support of my Family, especially my elder Father. I am deeply grateful to my Mother, Father, elder Father and Sisters for their love, care and all the sacrifice they made for my education.

関連したドキュメント