新技術説明会 ラマン分光 必見! AFM- ラマンによるナノイメージの世界 株式会社堀場製作所

Similar documents
2018 年 ( 平成 30 年 ) 7 月 13 日 ( 金曜日 ) Fri July 13, 2018

Agilent 4263B LCR Meter Operation Manual. Manual Change. Change 1 Add TAR in Test Signal Frequency Accuracy Test (Page 9-38) as follows.

BCR30AM-12LB. RJJ03G Rev I T(RMS) 30 A V DRM 600 V I FGT I, I RGT I, I RGT III 50 ma : PRSS0004ZE-A ( : TO-3P) 4 2, 4

むらの定量化について IEC-TC110 HHG2 への提案をベースに ソニー株式会社冨岡聡 フラットパネルディスプレイの人間工学シンポジウム

Thermal Safety Software (TSS) series

ROSE リポジトリいばらき ( 茨城大学学術情報リポジトリ )

galaxy science with GLAO

21 点 15 点 3 解答用紙に氏名と受検番号を記入し, 受検番号と一致したマーク部分を塗りつぶすこと 受検番号が 0( ゼロ ) から始まる場合は,0( ゼロ ) を塗りつぶすこと

C-H Activation in Total Synthesis Masayuki Tashiro (M1)

The unification of gravity and electromagnetism.

Yutaka Shikano. Visualizing a Quantum State

757G-V2 Series. For General Lighting Application. NF2x757G-F1, NFSx757G COB Series. Ra 90. Ra 80 Cove Light. Surface Mount Type

Scanning Probe Microscopy. Amanda MacMillan, Emmy Gebremichael, & John Shamblin Chem 243: Instrumental Analysis Dr. Robert Corn March 10, 2010

Reactive Fluid Dynamics 1 G-COE 科目 複雑システムのデザイン体系 第 1 回 植田利久 慶應義塾大学大学院理工学研究科開放環境科学専攻 2009 年 4 月 14 日. Keio University

一般化川渡り問題について. 伊藤大雄 ( 京都大学 ) Joint work with Stefan Langerman (Univ. Libre de Bruxelles) 吉田悠一 ( 京都大学 ) 組合せゲーム パズルミニ研究集会

京都 ATLAS meeting 田代. Friday, June 28, 13

TEOS characterization of 2D materials from graphene to TMDCs

Product Specification

Youhei Uchida 1, Kasumi Yasukawa 1, Norio Tenma 1, Yusaku Taguchi 1, Jittrakorn Suwanlert 2 and Somkid Buapeng 2

Listening Comprehension Sample 1

シミュレーション物理 6 運動方程式の方法 : 惑星の軌道 出席のメール ( 件名に学生番号と氏名 ) に, 中点法をサブルーチンを使って書いたプログラムを添付

Crustal Deformation Associated with the 2005 West Off Fukuoka Prefecture Earthquake Derived from ENVISAT/InSAR and Fault- slip Modeling

On Attitude Control of Microsatellite Using Shape Variable Elements 形状可変機能を用いた超小型衛星の姿勢制御について

質量起源 暗黒物質 暗黒エネルギー 宇宙線 陽子崩壊 ニュートリノ質量 米国 P5 ニュートリノ CPV 宇宙背景ニュートリノクォーク レプトンマヨラナ粒子 ニュートリノ測定器 陽子崩壊探索. Diagram courtesy of P5. Origin of Mass.

Improving Micro-Raman/AFM Systems Imaging Using Negative-Stiffness Vibration Isolation

Improving nano-scale imaging of of intergrated micro-raman/afm systems using negativestiffness

Hetty Triastuty, Masato IGUCHI, Takeshi TAMEGURI, Tomoya Yamazaki. Sakurajima Volcano Research Center, DPRI, Kyoto University

Relation of machine learning and renormalization group in Ising model

The most versatile AFM platform for your nanoscale microscopy needs

CMB の温度 偏光揺らぎにおける弱い重力レンズ効果 並河俊弥 ( 東京大学 )

Report on the experiment of vibration measurement of Wire Brushes. mounted on hand held power tools ワイヤ ブラシ取付け時の手持動力工具振動測定調査の実施について

LabRAM HR Evolution. Research Raman Made Easy!

D j a n g o と P H P の仲間たち ( 改変済 ) サイボウズ ラボ株式会社 TSURUOKA Naoya

日本政府 ( 文部科学省 ) 奨学金留学生申請書

Fast response silicon pixel detector using SOI. 2016/08/10 Manabu Togawa

Lecture 4 Scanning Probe Microscopy (SPM)

Analysis of shale gas production performance by SGPE

英語問題 (60 分 ) 受験についての注意 3. 時計に組み込まれたアラーム機能 計算機能 辞書機能などを使用してはならない 4. 試験開始前に 監督から指示があったら 解答用紙の受験番号欄の番号が自身の受験番号かどうかを確認し 氏名を記入すること

GRASS 入門 Introduction to GRASS GIS

Taking an advantage of innovations in science and technology to develop MHEWS

PROTEUS, AND THE NAME OF THE TYPE SPECIES OP THE GENUS HUENIA

Spontaneous magnetization of quark matter in the inhomogeneous chiral phase

Title rays. Citation Advanced Materials Research, 409: 5. Issue Date Journal Article. Text version author.

一体型地上気象観測機器 ( ) の風計測性能評価 EVALUATION OF WIND MEASUREMENT PERFORMANCE OF COMPACT WEATHER SENSORS

Day 5. A Gem of Combinatorics 組合わせ論の宝石. Proof of Dilworth s theorem Some Young diagram combinatorics ヤング図形の組合せ論

2015 年度研究活動報告理工学術院 先進理工 応用物理学科小澤徹 Department of Applied Physics, Waseda University

Fusion neutron production with deuterium neutral beam injection and enhancement of energetic-particle physics study in the Large Helical Device

EU 向けに輸出される食品等に関する証明書の発行に係る事務処理要領 ( 国際 ) 通知に基づき 欧州連合 ( 以下 EU という ) へ輸出される食品及び飼料の証明書の発行条件及び手続きを定めるものとする

ROSE リポジトリいばらき ( 茨城大学学術情報リポジトリ )

Illustrating SUSY breaking effects on various inflation models

NEW Ó Ó Ó Ó *VENT DETAIL X2 KNIGHT RIDER DARK SMOKE (C00) X2 GREY MATTER J.BLUE STEEL (C04) X2 INVERSE J.RED ION (C05) *ボーナスレンズ J.

Nanoscale Chemical Imaging with Photo-induced Force Microscopy

Bringing optics into the nanoscale a double-scanner AFM brings advanced optical experiments within reach

SPSS/SAS ANOVA Manual

2018 年度推薦入学選考 (11 月 15 日実施 ) 英語分野問題 ( 1 ページ 8 ページ )

XENON SHORT ARC LAMPS キセノンショートアークランプ

Reaction mechanism of fusion-fission process in superheavy mass region

車載用高効率燃焼圧センサー基板に最適なランガサイト型結晶の開発 結晶材料化学研究部門 シチズンホールディングス ( 株 )* 宇田聡 八百川律子 * Zhao Hengyu 前田健作 野澤純 藤原航三

谷本俊郎博士の研究業績概要 谷本俊郎博士は これまで地球内部の大規模なマントルの対流運動を解明するための研究 および 大気 - 海洋 - 固体地球の相互作用に関する研究を様々な角度から進めてきた これらのうち主要な研究成果は 以下の様にまとめることができる

Altitudinal Increasing Rate of UV radiation by the Observations with Brewer Spectrophotometers at Norikura, Suzuran and Tsukuba

Study of Cloud and Precipitation Processes Using a Global Cloud-system Resolving Model

新学習指導要領で求められる暗黙知の指導に関する事例研究 保健体育科教育法 Ⅰと器械運動 Ⅱにおける指導内容から

東ソー株式会社 - 明日のしあわせを化学する - TOSOH CORPORATION The Chemistry of Innovation. TOSOH CORPORATION The Chemistry of Innovation

マテリアルズインフォマティクスの最前線 吉田 亮. サイエンティフィック システム研究会 科学技術計算分科会 2017年度会合

11/13 Diagonalization. Theorem: The set R of all real numbers is not enumerable. 12/13. 0.a k1 a k2 a k3... where a ij {0, 1,...

Method for making high-quality thin sections of native sulfur

STM: Scanning Tunneling Microscope

NIE を取り入れた教育実践研究 大学 2 年生を対象とした時事教養 Ⅰ の授業実践を通して. Educational Research based on Newspaper In Education (NIE)

Evaluation of IGS Reprocessed Precise Ephemeris Applying the Analysis of the Japanese Domestic GPS Network Data

第 6 回 スペースデブリワークショップ 講演資料集 291 E3 デオービット用膜面展開機構の開発 Development of Membran Deployment mechanism for Deorbiting 高井元 ( 宇宙航空研究開発機構 ), 古谷寛, 坂本啓 ( 東京工業大学 ),

Combined AFM and Raman Enables: Comprehensive Data Using Optical, AFM, and Spectroscopic Methods

Introduction to Multi-hazard Risk-based Early Warning System in Japan

Oxford, Vol. 9, pp (2004).. (3) 微小空間を活用する多相系有機合成反応 小林重太 森雄一朗 小林修 化学と工業 59, pp (2006).

トンネルの切羽からの肌落ちによる 労働災害の調査分析と防止対策の提案

THE HOLISTIC LOVE REPORT

WHO 飲料水水質ガイドライン第 4 版 ( 一部暫定仮訳 ) 第 9 章放射線学的観点 9.4 飲料水中で一般的に検出される放射性核種のガイダンスレベル 過去の原子力緊急事態に起因する長期被ばく状況に関連する可能性のある人工の放射性核種のみならず 飲料水供給で最も一般的に検出される自然由来及び人工

Contents. What is AFM? History Basic principles and devices Operating modes Application areas Advantages and disadvantages

Other SPM Techniques. Scanning Probe Microscopy HT10

マスタタイトルの書式設定. Beyond ALMA. ALMA: 何がわかったか 何が足りないか LST: 何をやりたいか どのような計画か ALMA へのボーナス効果 最後に :small developments が未来を切り開く. Ryohei Kawabe (NAOJ)

NSPA510BS RoHS Compliant

The cause of the east west contraction of Northeast Japan

Fundamentals of nanoscience

Study of General Dynamic Modeling Using the Craig-Bampton Method

重力波天体の多様な観測による 宇宙物理学の新展開 勉強会 熱海 銀河における元素量の観測. 青木和光 Wako Aoki. 国立天文台 National Astronomical Observatory of Japan

Clark Atlanta University Center for Surface Chemistry and Catalysis Instrument Capabilities

Combining High Resolution Optical and Scanning Probe Microscopy

IAEA,NEA ISOE 国際 シンポジューム出張報告

Development of Advanced Simulation Methods for Solid Earth Simulations

Nanoscale IR spectroscopy of organic contaminants

Development of a High-Resolution Climate Model for Model-Observation Integrating Studies from the Earth s Surface to the Lower Thermosphere

NSPW500DS RoHS Compliant

スペース赤外線天文学の 現状と将来 ~ 波長の壁を越えて ~ 中川貴雄 (ISAS/JAXA)

EDL analysis for "HAYABUSA" reentry and recovery operation はやぶさ カプセル帰還回収運用における EDL 解析

高エネルギーニュートリノ : 理論的な理解 の現状

高分解能原子核乾板を用いた暗黒物質探索 中竜大 名古屋大学基本粒子研究室 (F 研 ) ICEPP 白馬

Optics and Spectroscopy

Introduction to Scanning Probe Microscopy Zhe Fei

-the 1st lecture- Yoshitaka Fujita Osaka University. Snake of March 16-20, 2015

CHARACTERIZATION of NANOMATERIALS KHP

Transcription:

新技術説明会 ラマン分光 必見! AFM- ラマンによるナノイメージの世界 株式会社堀場製作所

2013 HORIBA Scientific. All rights reserved. Ultra fast simultaneous AFM and hyper-spectral imaging: chemical and physical investigation of nano-materials made fast and easy. Ultra fast AFM- imaging Emmanuel Leroy AFM- Product Manager 256x256pts simultaneous topography and composite image of graphene Multi-modal imaging Microscopy today is much more than looking at a magnified image Multi-modal imaging Microscopy today is much more than looking at a magnified image It s about multiple ways of looking at a given sample. 1

Why AFM- Scanning Probe Microscopy (SPM) and specifically Atomic Force Microscopy (AFM) have made nanoscale imaging an affordable reality Cheaper than SEM and TEM Much less sample preparation. Very versatile Atomic Force Microscopy (AFM) came as an easier to use and flexible technique With AFM s popularity came many more modes of operation, providing much more than topography Elasticity / plasticity of materials, Young s modulus Conductivity/Resistivity (C-AFM), Surface Potential / Kelvin Probe (SKM, KPFM) Graphene on copper foil, AFM and KPFM images Magnetic Force (MFM) Why AFM- AFM, the most common SPM technique, is ideal for imaging physical parameters, but lacks sensitivity to chemical structure and composition 2

Spectroscopy: spectra to images Spectroscopy, especially IR and, are much better suited for label-free chemical analysis Spectroscopy: spectra to images but spectra are still pretty obscure for most people Spectroscopy: spectra to images People want things they can make sense of: people want images! Why AFM- AFM- brings chemical imaging and nanoscale physical characteristics imaging together. This is multi-modal imaging pushed beyond optical microscopy and to the nano scale Why TERS? spectroscopy brings highly specific chemical information, but spatial resolution is limited by Abbe s law of light diffraction. 12000 10000 8000 6000 4000 2000 876.0 1062.5 1128.3 1168.3 1264.1 1294.2 1369.4 1415.4 1439.5 1461.6 1641.5 0 800 1000 1200 1400 1600 Why TERS? Super-resolution techniques have brought chemical information down to ~30nm scale, but they all rely on fluorescent labels. SPM techniques can provide many physical properties at the nano scale (mechanical, electrical, magnetic ), but no chemical specificity Tip-Enhanced brings the prospect of label-free chemical imaging at the nano scale. Deckert et al. 2008 3

Instrumental Challenges Combining such different techniques as SPM and Spectroscopy is challenging. The common approach has been to perform co-localized measurements in sequence: First Spectroscopy to find an area of interest, then AFM for nanoscale characterization, or vice-versa: find a physical structure of interest to determine chemical structure with spectroscopy Challenges: Optics Tighter spot on the tip = better contrast Higher collection efficiency = better signal In order to illuminate the probe tip, there needs to be proper optical access for such high numerical aperture objective lens Challenges: Optics Tighter spot on the tip = better contrast The spot size is directly dependent on the NA as R = 0.6* /NA Challenges: Optics Higher collection efficiency = better signal The collection efficiency depends on the NA 2! Challenges: Optics & Sample Best solution: Inverted microscope SPM on top, bottom access for High NA objective up to 1.49 Samples need to be transparent 4

Challenges: Optics & Sample For opaque samples: Top illumination can accept fairly high NA objectives (0.7) Shadowing from the cantilever is an issue and the probe needs to be protruded Challenges: AFM diode It is also important to note that the AFM feedback requires a diode laser, which may interfere with the spectroscopy measurements: An AFM diode in the IR is required to perform AFM- in the full range of VIS-NIR lasers available. The diode must not use the same beam path as the spectroscopy laser, or independent alignment becomes very cumbersome Fast simultaneous AFM- IR AFM Diode (no interference) Access to change sample and tip without moving the head Auto-cantilever alignment and tuning (comes back to the same place) Top access with 0.7NA objective, side access with up to 0.7NA for TERS Visual confirmation of alignment in all ports Fast simultaneous AFM- Powerful software package 1300nm Auto alignment Video viewing of tip and laser Easy tip exchange High NA access IR AFM Diode (no interference) Access to change sample and tip without moving the head Auto-cantilever alignment and tuning (comes back to the same place) Top access with 0.7NA objective, side access with up to 0.7NA for TERS Visual confirmation of alignment in all ports Integrated multivariate module High level analysis at a touch of a button PCA MCR HCA DCA KnowItAll HORIBA Edition Fast chemical identification HORIBA spectral database (>1750 spectra) 5

Added advantage Not only integrates a powerful, high resolution AFM, with high frequency scanner, little sensitive to vibrations Also combines powerful microscope that can be used as standalone (3 instruments in one) Added advantage: real-time autofocus The AFM also acts as an autofocus in real time, therefore it is possible to measure samples with very high topography without worrying about depth of focus and the sample going in and out of focus no need for additional pass to measure topography or additional hardware, it is all included! A nice added feature Conclusions Tight integration between a SPM system designed for spectroscopy and a powerful micro-spectrometer brings efficient, ultra fast multi-modal imaging to characterize nano materials High spatial resolution and speed is achieved thanks to open access from the top with high NA optics, and lack of interference from the AFM. Lipid layer: and AFM topography 30x30um scan 7um topography Conclusions Suited for TERS with side access port for best polarization and collection efficiency Long term stability insured thanks to rugged, inovative, automated alignment features making it easy to use. Conclusions Experience the most versatile, easy-to-use, and fast simultaneous AFM- system For more information come to our booth # 6 2013 HORIBA, Ltd. All Right Reserved 無断転載 複写複製について本資料の内容の一部あるいは全部を当社の許可なく無断で転載したり変更したりすることは 固くお断りします