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  1. NTU Theses and Dissertations Repository
  2. 理學院
  3. 物理學系
請用此 Handle URI 來引用此文件: http://tdr.lib.ntu.edu.tw/jspui/handle/123456789/50478
完整後設資料紀錄
DC 欄位值語言
dc.contributor.advisor陳永芳
dc.contributor.authorYu-Ming Liauen
dc.contributor.author廖佑銘zh_TW
dc.date.accessioned2021-06-15T12:42:27Z-
dc.date.available2026-12-31
dc.date.copyright2016-10-14
dc.date.issued2016
dc.date.submitted2016-07-27
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dc.identifier.urihttp://tdr.lib.ntu.edu.tw/jspui/handle/123456789/50478-
dc.description.abstract隨機雷射比起傳統雷射擁有許多先天的優勢像是裝置可彎曲性、微小體積、低成本、設計簡單以及量產的可能性。隨機雷射已經在近十年成為非常熱門的研究領域。我們的隨機雷射標籤整合了隨意轉貼在各種非傳統基板的製程設計、可彎曲的材質以及溫度感測的功能於單一裝置。超薄隨機雷射標籤不僅僅可以持續穩定地在500 次以上拉伸壓縮100 %的嚴苛條件下繼續正常運作,甚至還可以用簡易的製程方法轉移到任意的基板不管是彎曲、非平面以及粗糙的材料上面。除了上面所述的功能之外,超薄隨機雷射標籤還可以用於人類體溫的感測。超薄隨機雷射標籤這樣的先進的光學裝置有很大的潛力在許多各式各樣的領域上運用。zh_TW
dc.description.abstractRandom lasers have abundant inherent advantages compared to conventional lasers such as flexibility, size, cost, simple design, and mass production. It has been the hot research topic in recent decades. An integrated random laser label with transferability, flexibility and temperature sensing is created and demonstrated in this
work. The ultrathin stick-type random laser (USRL) can not only function stably under 100% strain with at least 500 times test but could also be easily transferred on arbitrary substrates disregard the material is rigid, flexible, non-planar or rough. In addition to features mentioned above, random laser signals could be stimulated and controlled repetitively within human body temperature. This shows great potential that the USRL can serve as photonics modules for further advanced developments of a variety of applications covering many different fields.
en
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Previous issue date: 2016
en
dc.description.tableofcontents口試委員會審定書........................................................................................................... I
誌謝 ................................................................................................................................. II
中文摘要 ........................................................................................................................ IV
Abstract ...........................................................................................................................V
List of Publication......................................................................................................... VI
Contents....................................................................................................................... VII
List of Figures ............................................................................................................... IX
Figure of chapter2................................................................................................. IX
Figure of chapter3...................................................................................................X
Figure of chapter4...................................................................................................X
Chapter1 Introduction ................................................................................................... 1
Reference ................................................................................................................. 4
Chapter 2 Theoretical Background............................................................................... 6
2.1 Band Gap Structure ......................................................................................... 6
2.2 Photoluminescence (PL) ................................................................................... 9
2.3 Random Laser (RL)........................................................................................ 12
2.3.1 Mechanisms .............................................................................................. 12
2.3.2 Unique Characters................................................................................... 13
2.3.3 Application ............................................................................................... 14
(1) Optomicrofluidics ..................................................................................... 14
(2) Cancer diagnostic...................................................................................... 16
(3) Speckle free imaging................................................................................. 17
(4) On-chip random spectrometer................................................................... 19
(5) Next generation light source ..................................................................... 21
2.4 Fabry–P eacute;rot resonance .................................................................................. 22
Reference ............................................................................................................... 23
Chapter 3 Experimental Details .................................................................................. 25
3.1 Scanning Electron Microscopy (SEM).......................................................... 25
3.2 Random Laser Measurement ........................................................................ 27
Reference ............................................................................................................... 28
Chapter 4 ....................................................................................................................... 29
Transferable, Highly Stretchable and Ultrathin Label-like Random Laser on
Universal Substrates..................................................................................................... 29
4.1 Introduction .................................................................................................... 29
4.2 Experimental Section ..................................................................................... 31
4.3 Result and Discussions ................................................................................... 32
4.4 Conclusion ....................................................................................................... 39
Reference ............................................................................................................... 50
Chapter 5 Conclusion ................................................................................................... 51
Figure 2. 1 Electronic band gap structure of metal, semiconductor, and
insulator material........................................................................................... 8
Figure 2. 2 (a) A direct optical transition is drawn vertically with no
change of k. (b) The indirect transition involves both a photon and a
phonon. .......................................................................................................... 8
Figure 2. 3 Illustration of an electronic transition corresponding with
absorption, spontaneous emission, and stimulated emission. ..................... 11
Figure 2. 4 (a) A 300 μm long pump stripe is translated along the length of
the channel, varying d, to study the spectral sensitivity of the random
lasing modes to the pumped region. The spectra recorded for three
different values of d are plotted in (b)......................................................... 15
Figure 2. 5 (Color) Random laser emission spectra of human colon tissues
infiltrated with a concentrated laser dye, namely R6G. (a) Two typical
random laser emission spectra from a healthy, grossly uninvolved tissue
(blue), of which microscopic image is shown in (b). The narrow spectral
lines are in fact coherent laser emission modes. The inset shows
schematically closed random laser resonators formed due to scatterers in
the gain medium. (c) and (d), same as in (a) and (b), respectively, but for a
malignant colon tissue. There are more lines in the laser emission spectra
in (c) (red) that are due to more resonators in the tumor; these are caused
by the excess disorder that is apparent in (d). ............................................. 16
Figure 2. 6 Random lasers, a new kind of light source for imaging. Light
sources are compared in terms of the two parameters most relevant to
full-field imaging: photon degeneracy/spectral radiance and spatial
coherence. Random lasers represent a new class of light source with high
photon degeneracy/spectral radiance and low spatial coherence—the ideal
combination for full-field imaging.............................................................. 18
Figure 2. 7 SEM image of the fabricated spectrometer. The dispersive
element is a semicircular array of randomly positioned air holes,
surrounded by a photonic-crystal lattice. The probe signal is coupled to the
random structure via a defect waveguide at the bottom of the semicircle.
The light then diffuses through the random array via multiple scattering
and eventually reaches the 25 defect waveguides around the circumference
of the semicircle. These tapered waveguides will couple the signals to the
doi:10.6342/NTU201601330
X
detectors (not integrated). The distribution of intensities over the detectors
is used to identify the input spectrum. The photonic-crystal boundary,
which has a full bandgap in two dimensions, confines the probe light in
the random structure and channels it efficiently into the defect waveguides.
The insets in the bottom row are magnified images, and the scale bars
indicate 1 mm. ............................................................................................. 20
Figure 2. 8 Schematic illustration of plane-parallel cavity. ....................... 22
Figure of chapter3
Figure 3. 1 Schematic diagram of a scanning electron microscope (SEM).26
Figure 3. 2 Picture of a scanning electron microscope (SEM). ................. 26
Figure 3. 3 Schematic illustration for the measurement of random lasing.27
Figure 3. 4 Picture of instrument for the measurement of random lasing. 28
Figure of chapter4
Figure 4. 1 Top view SEM image of ZnO nanoparticles. .......................... 40
Figure 4. 2 Schematic fabrication process of the USRL. ........................... 41
Figure 4. 3 Top view of the USRL separating from the silicon substrate
and floating on the DI water. ....................................................................... 42
Figure 4. 4 (a) Evolution of emission peak intensity as a function of
pumping energy on the silicon substrate. The inset is a schematic diagram
showing the formation of closed-loop paths for light though multiple
scattering by ZnO nanoparticles suspended in PMMA film. (b) Emission
spectrum as a function of pumping energy for the USRL on the silicon
substrate. (c) Evolution of emission peak intensity as a function of
pumping energy on the PET substrate. The inset is the photograph of the
sample (top view). (d) Emission spectrum as a function of pumping energy
for the USRL on the PET substrate. ............................................................ 43
Figure 4. 5 Emission peak intensity as a function of the USRL under
different emission angles from 25 to 65 degree. ......................................... 44
Figure 4. 6 (a-e) Demonstrations of the USRL labelled onto various
non-conventional substrates with the corresponding evolution of emission
peak intensity and emission spectrum as a function of pumping energy
alongside, including on a glass bottle (a), a glove (b), a peelable Post-it
flag (c), a scotch tape (d), a paper money (e). (The areas of the USRLs are
about 1.5 cm2.)............................................................................................. 45
Figure 4. 7 (a) The USRL was clipped on the slide caliper under
compressing from 0 % to 50 % and re-stretching from 0 % strain to 100 %
strain, and the corresponding emission spectrum and evolution of emission
doi:10.6342/NTU201601330
XI
peak intensity as a function of pumping energy under different
compression. (b) The SEM image of the USRL under pre-strain and after
releasing pre-strain. ..................................................................................... 46
Figure 4. 8 Emission spectrum as a function of the USRL under different
compressing cycles from 100 times to 500 times. ...................................... 47
Figure 4. 9 (a) Emission spectrum as a function of the USRL under
different temperature. (b) Demonstrations of emission spectra of the USRL
labelled onto glass bottle filled in dissimilar temperature water................. 48
Figure 4. 10 Emission spectrum as a function of the USRL under different
temperatures. ............................................................................................... 49
dc.language.isoen
dc.subject可拉伸zh_TW
dc.subject可轉移zh_TW
dc.subject隨機雷射zh_TW
dc.subject氧化鋅奈米粒子zh_TW
dc.subject超薄zh_TW
dc.subject可彎曲zh_TW
dc.subjectUltrathinen
dc.subjectRandom Lasersen
dc.subjectStretchableen
dc.subjectTransferrableen
dc.subjectFlexibleen
dc.subjectZnO Nanoparticlesen
dc.subjectUltrathinen
dc.subjectRandom Lasersen
dc.subjectStretchableen
dc.subjectTransferrableen
dc.subjectFlexibleen
dc.subjectZnO Nanoparticlesen
dc.title可轉貼可高度拉伸超薄隨機雷射標籤在各種基板之光
學研究分析與應用演示
zh_TW
dc.titleTransferable, Highly Stretchable and Ultrathin Label-like
Random Laser on Universal Substrates
en
dc.typeThesis
dc.date.schoolyear104-2
dc.description.degree碩士
dc.contributor.oralexamcommittee林泰源,許芳琪
dc.subject.keyword隨機雷射,可拉伸,可轉移,可彎曲,氧化鋅奈米粒子,超薄,zh_TW
dc.subject.keywordRandom Lasers,Stretchable,Transferrable,Flexible,ZnO Nanoparticles,Ultrathin,en
dc.relation.page51
dc.identifier.doi10.6342/NTU201601330
dc.rights.note有償授權
dc.date.accepted2016-07-27
dc.contributor.author-college理學院zh_TW
dc.contributor.author-dept物理學研究所zh_TW
顯示於系所單位:物理學系

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