JPH06100544B2 - Laser emission spectroscopy analyzer - Google Patents

Laser emission spectroscopy analyzer

Info

Publication number
JPH06100544B2
JPH06100544B2 JP61162478A JP16247886A JPH06100544B2 JP H06100544 B2 JPH06100544 B2 JP H06100544B2 JP 61162478 A JP61162478 A JP 61162478A JP 16247886 A JP16247886 A JP 16247886A JP H06100544 B2 JPH06100544 B2 JP H06100544B2
Authority
JP
Japan
Prior art keywords
light
light emitted
spectroscope
laser
laser emission
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired - Fee Related
Application number
JP61162478A
Other languages
Japanese (ja)
Other versions
JPS6318249A (en
Inventor
亘 谷本
山本  公
Original Assignee
川崎製鉄株式会社
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by 川崎製鉄株式会社 filed Critical 川崎製鉄株式会社
Priority to JP61162478A priority Critical patent/JPH06100544B2/en
Publication of JPS6318249A publication Critical patent/JPS6318249A/en
Publication of JPH06100544B2 publication Critical patent/JPH06100544B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N21/00Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
    • G01N21/62Systems in which the material investigated is excited whereby it emits light or causes a change in wavelength of the incident light
    • G01N21/71Systems in which the material investigated is excited whereby it emits light or causes a change in wavelength of the incident light thermally excited
    • G01N21/718Laser microanalysis, i.e. with formation of sample plasma

Landscapes

  • Health & Medical Sciences (AREA)
  • Physics & Mathematics (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Plasma & Fusion (AREA)
  • Optics & Photonics (AREA)
  • Nuclear Medicine, Radiotherapy & Molecular Imaging (AREA)
  • Engineering & Computer Science (AREA)
  • Chemical & Material Sciences (AREA)
  • Analytical Chemistry (AREA)
  • Biochemistry (AREA)
  • General Health & Medical Sciences (AREA)
  • General Physics & Mathematics (AREA)
  • Immunology (AREA)
  • Pathology (AREA)
  • Investigating, Analyzing Materials By Fluorescence Or Luminescence (AREA)

Description

【発明の詳細な説明】Detailed Description of the Invention 【産業上の利用分野】[Industrial applications]

本発明は、レーザ発光分光分析装置に係り、特に、微量
成分分析に用いるのに好適な、試料にレーザ光を照射し
た時に放出される光を分光器でスペクトルに分離し、各
元素のスペクトル強度より成分元素を定量分析するレー
ザ発光分光分析装置の改良に関する。
TECHNICAL FIELD The present invention relates to a laser emission spectroscopic analyzer, and in particular, it is suitable for use in trace component analysis, and separates light emitted when a sample is irradiated with laser light into a spectrum by a spectroscope to obtain spectral intensity of each element. The present invention relates to improvement of a laser emission spectroscopic analysis device for quantitatively analyzing component elements.

【従来の技術】 近年レーザ技術の進歩と共に、これを分光分析の励起源
として利用する各試みが各方面で進められている。この
ような試みにおいては、例えば第3図に示す如く、試料
10の表面に適当な集光レンズ12によつて焦点を結ぶよう
にされた強力なレーザ光をレーザ発振器14から照射し
て、試料10の表面層を急速に加熱する。特に、レーザ光
が数十nsecのパルス状であると、試料内部へ熱が拡散す
る前に局所的にエネルギが注入された状態となり、試料
10の表面層で融解及び蒸発が起こる。蒸気は、レーザ光
によつて更に励起されてプラズマ16となり光を放出す
る。 このプラズマ16から放出される光を適当な光導入系18
(第3図では集光鏡19を含む)を用いて分光器20に伝送
し、回折格子22等により分光してスペクトルに分離した
後、各元素のスペクトル強度を写真フイルム、光電子増
倍管24、フオトダイオード等により検出することによつ
て、目的元素の含有量を調べるようにされている。図に
おいて、26は分光器の入射スリツト、28は反射鏡、30は
出射スリツト、32は信号処理器、34は計算機である。 このようなレーザ発光分光分析方法は、試料10の非接触
で分析が可能であり、試料10が非導電性物質でも、溶融
状態にあつても分析できるという利点がある半面、信号
対バツクグラウンド比(以下S/B比と称する)が悪く、
分析精度及び正確度が著しく劣るという欠点を有してい
た。これは、レーザ光照射によつて生成されたプラズマ
16からは、各元素スペクトルと共に連続光も放出されて
おり、この連続光が本手法におけるバツクグラウンドの
主な要因となつているためである。 この連続光を除去するものとして、出願人は既に特開昭
57−100323を開示している。これは、レーザ光照射直後
のプラズマからは、まず連続光を主成分とした光が放出
され、次いで元素スペクトルが放出されるという知見に
基づき、測定を時間的に分離して、レーザ光照射から1
μsec経過後、該レーザ光照射から16μsec経過するまで
の時間に放出される光を分光分析することにより、S/B
比の向上を図つたものである。
2. Description of the Related Art With the progress of laser technology in recent years, various attempts have been made in various fields to utilize it as an excitation source for spectroscopic analysis. In such an attempt, for example, as shown in FIG.
The surface of the sample 10 is rapidly heated by irradiating the surface of the sample 10 with a strong laser beam focused by a suitable condenser lens 12 from a laser oscillator 14. In particular, if the laser light is pulsed for several tens of nanoseconds, energy will be locally injected before heat is diffused into the sample,
Melting and evaporation occur in 10 surface layers. The vapor is further excited by laser light to become plasma 16 and emits light. The light emitted from the plasma 16 is converted into an appropriate light introduction system 18
After being transmitted to the spectroscope 20 using a condensing mirror 19 (in FIG. 3) and separated into spectra by the diffraction grating 22 or the like, the spectral intensities of the respective elements are photographed film, photomultiplier tube 24. The content of the target element is examined by detecting with a photo diode or the like. In the figure, 26 is an entrance slit of the spectroscope, 28 is a reflecting mirror, 30 is an exit slit, 32 is a signal processor, and 34 is a calculator. Such a laser emission spectroscopic analysis method enables analysis without contacting the sample 10, and has the advantage that the sample 10 can be analyzed even when it is a non-conductive substance or in a molten state, while the signal-to-background ratio is high. (Hereinafter referred to as S / B ratio) is bad,
It had a drawback that the analysis accuracy and precision were extremely poor. This is the plasma generated by laser light irradiation.
This is because continuous light is emitted from 16 along with each element spectrum, and this continuous light is the main cause of the background in this method. The applicant has already proposed that the continuous light should be removed.
57-100323 is disclosed. This is because, based on the knowledge that the light mainly composed of continuous light is emitted from the plasma immediately after the laser light irradiation, and then the element spectrum is emitted, the measurement is temporally separated and the laser light irradiation is performed. 1
After the elapse of μsec, the light emitted during the period from the irradiation of the laser beam to the elapse of 16 μsec is spectroscopically analyzed to obtain S / B.
This is intended to improve the ratio.

【発明が解決しようとする問題点】[Problems to be Solved by the Invention]

しかしながら、この時間分解測定法による連続光の除去
においては、次のような問題点を有していた。即ち、連
続光と元素スペクトルは、その放出時間が一部重なつて
いるため、これを精度良く分離するためには、数十nsec
程度の非常に高速なゲート回路や高速応答光検出器等の
特殊な装置が必要となる。又、元素スペクトルよりも連
続光の方が強度が大きいため、光検出器、増幅器のゲイ
ンが連続光のピーク強度で制限されてしまう。従つて、
例えば微量元素スペクトルを測定する場合、感度を上げ
るためにゲインを大きくしても、連続光のピーク強度で
各素子が飽和してしまい、微量成分元素に対して充分な
感度が得られず、必要なゲインまで大きくすることがで
きない。よつて、分析精度をある程度までしか向上する
ことができず、特に微量成分分析時に、充分な感度や精
度が得られないという問題点を有していた。 一方、特開昭58−219438には、試料にレーザ光を照射し
て形成されたプラズマから放出される光を、中心部に穴
を開け、周辺部を反射面としたリング状の集光鏡により
分光器に導入することが記載されているが、リング状の
集光鏡を用いた場合には、レーザの光軸と受光の光軸を
精度良く同軸に合せるための厳密な光軸調整が必要であ
り、且つ、鏡面(通常アルミニウムの蒸着膜)が長時間
使用時に試料からの蒸発物質等により汚れるため、クリ
ーニングする必要があるが、傷がつき易いので保守も大
変であるという問題点を有していた。 本発明は、前記従来の問題点を解消するべくなされたも
ので、高速応答素子等の特殊な装置や厳密な光軸調整を
必要とすることなく、簡単な保守で、微量成分分析時に
も充分な感度及び精度が得られるレーザ発光分光分析方
法及び装置を提供することを目的とする。
However, the removal of continuous light by this time-resolved measurement method has the following problems. That is, the emission times of continuous light and elemental spectra partially overlap with each other.
A special device such as a very high speed gate circuit or a high speed response photodetector is required. Further, since the intensity of continuous light is higher than that of the element spectrum, the gains of the photodetector and the amplifier are limited by the peak intensity of continuous light. Therefore,
For example, when measuring a trace element spectrum, even if the gain is increased to increase the sensitivity, each element is saturated with the peak intensity of continuous light, and sufficient sensitivity cannot be obtained for trace element elements. It is not possible to increase the gain. Therefore, there has been a problem that the analysis accuracy can be improved only to some extent, and sufficient sensitivity and accuracy cannot be obtained especially when a trace component analysis is performed. On the other hand, Japanese Patent Laid-Open No. 58-219438 discloses a ring-shaped condensing mirror which has a hole at the center and a reflection surface at the periphery for light emitted from plasma formed by irradiating a sample with laser light. However, when a ring-shaped condenser mirror is used, strict optical axis adjustment is required to accurately align the optical axis of the laser and the optical axis of the received light coaxially. It is necessary and needs to be cleaned because the mirror surface (usually a vapor deposition film of aluminum) is contaminated by evaporative substances from the sample when used for a long time, but it is easily scratched and difficult to maintain. Had. The present invention has been made to solve the above-mentioned conventional problems, does not require a special device such as a high-speed response element or strict optical axis adjustment, is simple in maintenance, and is sufficient even for trace component analysis. It is an object of the present invention to provide a laser emission spectroscopic analysis method and device that can obtain various sensitivities and precisions.

【問題点を解決するための手段】[Means for solving problems]

本発明は、試料にレーザ光を照射した時に放出される光
を分光器でスペクトルに分離し、各元素のスペクトル強
度より成分元素を定量分析するレーザ発光分光分析装置
において、前記放出光を分光器に導入する光導入系に、
試料表面上に形成されるプラズマのうち、中心部から放
出される光を除き、周辺部から放出される光だけを選択
的に分光器に導入する光選択手段として、中心部に透過
防止処理が施され、周辺部に透過処理が施された集光レ
ンズを設けることにより、前記目的を達成したものであ
る。 又、本発明の他の実施態様は、前記光選択手段を、前記
集光レンズに代えてスリツトとしたものである。
The present invention relates to a laser emission spectroscopic analyzer that separates light emitted when a sample is irradiated with laser light into a spectrum with a spectroscope and quantitatively analyzes component elements from the spectral intensities of the respective elements. The light introduction system to be introduced into
Among the plasma formed on the sample surface, the light emitted from the central part is excluded, and only the light emitted from the peripheral part is selectively introduced into the spectroscope as a light selection means. The above object is achieved by providing a condensing lens which is provided and which has been subjected to a transmission treatment in the peripheral portion. In another embodiment of the present invention, the light selecting means is a slit instead of the condenser lens.

【作用】[Action]

発明者らが、前出第3図に示した装置において、試料1
0、光導入系18及び分光器20を固定しておいて、レーザ
光軸を移動することにより、プラズマ16の中心部及び周
辺部から放出される光を測定したところ、プラズマ中心
部からはバツクグラウンドとなる連続光が主に放出され
ているのに対して、プラズマ周辺部では連続系の放出は
極めて小さく分光分析に使用する元素スペクトルが主に
放出されていることを見出した。 本発明は、このような知見に基づいてなされたもので、
試料にレーザ光を照射した時に放出される光を分光器で
スペクトルに分離し、各元素のスペクトル強度より成分
元素を定量分析するに際して、試料表面上に形成される
プラズマのうち、中心部から放出される光を除き、周辺
部から放出される光だけを選択的に分光器に導入して分
光分析を行うようにしている。従つて、S/B比が向上
し、高速応答素子等の特殊な装置を必要とすることな
く、微量成分分析時にも充分な感度や精度を得ることが
できる。 ここで、スリツトだけでなく、中心部に透過防止処理が
施された集光レンズによつても、プラズマ中心部からの
放出光のみを除くことができるのは、プラズマが理論的
な点光源ではなく、ある大きさ(約3mm径)を有してい
るからである。即ち、プラズマ中の放出光の位置と分光
器の入射スリツト及び集光レンズの透過防止処理部相互
間の幾何学的な位置関係により、プラズマ中心部からの
放出光が分光器に取込まれなくなる。
In the device shown in FIG.
0, the light introduction system 18 and the spectroscope 20 are fixed, and the laser light axis is moved to measure the light emitted from the central portion and the peripheral portion of the plasma 16. It was found that continuous light, which is the ground, is mainly emitted, whereas continuous system emission is extremely small in the peripheral part of the plasma, and the element spectrum used for spectroscopic analysis is mainly emitted. The present invention was made based on such findings,
The light emitted when the sample is irradiated with laser light is separated into spectra with a spectroscope, and when quantitatively analyzing the constituent elements from the spectral intensity of each element, the plasma is emitted from the center of the plasma formed on the sample surface. The emitted light is excluded and only the light emitted from the peripheral portion is selectively introduced into the spectroscope for spectroscopic analysis. Therefore, the S / B ratio is improved, and sufficient sensitivity and accuracy can be obtained even in the analysis of a trace amount of components, without requiring a special device such as a high-speed response element. Here, not only the slit but also the condensing lens having the central portion subjected to the anti-transmission treatment can eliminate only the light emitted from the central portion of the plasma in the point source where plasma is theoretical. Instead, it has a certain size (about 3 mm diameter). That is, due to the geometrical positional relationship between the position of the emitted light in the plasma, the incident slit of the spectroscope, and the transmission prevention processing section of the condenser lens, the emitted light from the central part of the plasma is not taken into the spectroscope. .

【実施例】【Example】

以下図面を参照して、本発明の実施例を詳細に説明す
る。 本発明の第1実施例は、第1図に示す如く、前出第3図
に示した従来例と同様のレーザ発光分光分析装置におい
て、前記光導入系18の集光鏡19の代りに、第1図に示す
如く、レンズの中心部に例えば塗料を塗ることによって
中心部に透過防止処理が施され、周辺部に透過処理が施
された集光レンズ42を設けたものである。他の点につい
ては前記従来例と同様であるので説明は省略する。 以下第1実施例の作用を説明する。 レーザ発振器14から放出されたレーザ光は集光レンズ12
で試料10の表面に集光照射される。レーザ光照射により
励起発光した光は、光導入系18の集光レンズ42で分光器
20の入射スリツト26に結像され、分光器20に導入され
る。この際、集光レンズ42により、プラズマ周辺部から
放出された光のみ分光器20に導入され、一方、プラズマ
中心部から放出された光は集光レンズ42の中心部を透過
できず、分光器20には導入されない。 分光器20に導入された光は、回折格子22によりスペクト
ルに分離され、出射スリツト30で所定元素のスペクトル
が選別され、光電子増倍管24でスペクトル強度が電気信
号に変換される。該電気信号は信号処理器32で増幅、積
算、アナログ−デジタル変換され、計算機34へ送られ
る。計算機34は、信号処理器32から送られてきた値と、
予め作成しておいた検量線より試料10中の元素濃度を算
出する。 次に、本発明の第2実施例を詳細に説明する。 この第2実施例は、第2図に示す如く、前記第1実施例
と同様のレーザ発光分光分析装置において、光導入系18
を、試料面上に設けられた、プラズマ中心部から放出さ
れる光を除き、その周辺部から放出される光のみを通過
させるスリツト44と、集光レンズ46とで構成したもので
ある。 他の点については前記第1実施例と同様であるので説明
は省略する。 本実施例によれば、構成が非常に簡略であり、本発明の
適用が容易である。
Embodiments of the present invention will be described in detail below with reference to the drawings. As shown in FIG. 1, the first embodiment of the present invention is similar to the prior art example shown in FIG. 3 in the laser emission spectroscopic analyzer, but instead of the condenser mirror 19 of the light introducing system 18, As shown in FIG. 1, a condensing lens 42 is provided in which the central portion of the lens is subjected to a permeation-preventing treatment and the peripheral portion thereof is permeating-treated by applying, for example, paint. Since the other points are the same as those of the conventional example, description thereof will be omitted. The operation of the first embodiment will be described below. The laser light emitted from the laser oscillator 14 is focused by the condenser lens 12
Then, the surface of the sample 10 is focused and irradiated. The light excited and emitted by the laser light irradiation is spectroscoped by the condenser lens 42 of the light introduction system 18.
An image is formed on the incident slit 26 of 20 and is introduced into the spectroscope 20. At this time, only the light emitted from the peripheral portion of the plasma is introduced into the spectroscope 20 by the condenser lens 42, while the light emitted from the central portion of the plasma cannot pass through the central portion of the condenser lens 42, and Not introduced in 20. The light introduced into the spectroscope 20 is separated into a spectrum by the diffraction grating 22, the spectrum of a predetermined element is selected by the exit slit 30, and the spectrum intensity is converted into an electric signal by the photomultiplier tube 24. The electric signal is amplified, integrated and analog-digital converted by the signal processor 32, and sent to the computer 34. The calculator 34 has the value sent from the signal processor 32,
The element concentration in Sample 10 is calculated from the calibration curve prepared in advance. Next, a second embodiment of the present invention will be described in detail. As shown in FIG. 2, this second embodiment is the same as the first embodiment except that the light introducing system 18 is used in the laser emission spectrum analyzer.
Is composed of a slit 44, which is provided on the surface of the sample, for passing only the light emitted from the peripheral portion of the plasma excluding the light emitted from the plasma central portion, and a condenser lens 46. Since the other points are the same as those in the first embodiment, the description thereof will be omitted. According to this embodiment, the configuration is very simple and the present invention can be easily applied.

【発明の効果】【The invention's effect】

以上説明した通り、本発明によれば、プラズマ放出光を
空間的に分離してS/B比を向上させているので、分析感
度が高く、微量成分分析時にも充分な感度や精度を得る
ことができるという優れた効果を有する。
As described above, according to the present invention, the plasma emission light is spatially separated to improve the S / B ratio, so that the analysis sensitivity is high, and sufficient sensitivity and accuracy can be obtained even in the analysis of trace components. It has an excellent effect that

【図面の簡単な説明】[Brief description of drawings]

第1図は、本発明に係るレーザ発光分光分析装置の第1
実施例の全体構成を示す、一部断面図を含む光路図、第
2図は、本発明の第2実施例の要部構成を示す、一部断
面図を含む光路図、第3図は、従来のレーザ発光分光分
析装置の構成例を示す、一部断面図を含む光路図であ
る。 10…試料、 14…レーザ発振器、 16…プラズマ、 18…光導入系、 20…分光器、 42…集光レンズ、 44…スリツト。
FIG. 1 is a first diagram of a laser emission spectroscopic analyzer according to the present invention.
FIG. 2 is an optical path diagram including a partial cross-sectional view showing the overall configuration of the embodiment, FIG. 2 is an optical path diagram including a partial cross-sectional view showing the configuration of a main part of a second embodiment of the present invention, and FIG. It is an optical-path figure which shows the structural example of the conventional laser emission spectroscopy analyzer including a partial cross section figure. 10 ... Sample, 14 ... Laser oscillator, 16 ... Plasma, 18 ... Light introducing system, 20 ... Spectroscope, 42 ... Condensing lens, 44 ... Slit.

Claims (2)

【特許請求の範囲】[Claims] 【請求項1】試料にレーザ光を照射した時に放出される
光を分光器でスペクトルに分離し、各元素のスペクトル
強度より成分元素を定量分析するレーザ発光分光分析装
置において、 前記放出光を分光器に導入する光導入系に、 試料表面上に形成されるプラズマのうち、中心部から放
出される光を除き、周辺部から放出される光だけを選択
的に分光器に導入する光選択手段として、中心部に透過
防止処理が施され、周辺部に透過処理が施された集光レ
ンズが設けられていることを特徴とするレーザ発光分光
分析装置。
1. A laser emission spectroscopic analyzer that separates the light emitted when a sample is irradiated with laser light into a spectrum with a spectroscope and quantitatively analyzes the constituent elements from the spectral intensity of each element. A light selection system that selectively introduces only the light emitted from the peripheral part of the plasma formed on the sample surface, excluding the light emitted from the central part, into the spectroscope in the light introduction system that is introduced into the instrument. The laser emission spectrum analyzer according to claim 1, further comprising a condensing lens which is subjected to a transmission preventing treatment in a central portion and which is subjected to a transmitting treatment in a peripheral portion.
【請求項2】試料にレーザ光を照射した時に放出される
光を分光器でスペクトルに分離し、各元素のスペクトル
強度より成分元素を定量分析するレーザ発光分光分析装
置において、 前記放出光を分光器に導入する光導入系に、 試料表面上に形成されるプラズマのうち、中心部から放
出される光を除き、周辺部から放出される光だけを選択
的に分光器に導入する光選択手段として、スリツトが設
けられていることを特徴とするレーザ発光分光分析装
置。
2. A laser emission spectroscopic analyzer that separates the light emitted when a sample is irradiated with laser light into a spectrum by a spectroscope and quantitatively analyzes the component elements from the spectral intensity of each element. A light selection system that selectively introduces only the light emitted from the peripheral part of the plasma formed on the sample surface, excluding the light emitted from the central part, into the spectroscope in the light introduction system that is introduced into the instrument. And a slit is provided as a laser emission spectrum analyzer.
JP61162478A 1986-07-10 1986-07-10 Laser emission spectroscopy analyzer Expired - Fee Related JPH06100544B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP61162478A JPH06100544B2 (en) 1986-07-10 1986-07-10 Laser emission spectroscopy analyzer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP61162478A JPH06100544B2 (en) 1986-07-10 1986-07-10 Laser emission spectroscopy analyzer

Publications (2)

Publication Number Publication Date
JPS6318249A JPS6318249A (en) 1988-01-26
JPH06100544B2 true JPH06100544B2 (en) 1994-12-12

Family

ID=15755380

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61162478A Expired - Fee Related JPH06100544B2 (en) 1986-07-10 1986-07-10 Laser emission spectroscopy analyzer

Country Status (1)

Country Link
JP (1) JPH06100544B2 (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
FR2706614B1 (en) * 1993-06-15 1995-07-13 Commissariat Energie Atomique Method of isotopic analysis by optical emission spectrometry on plasma produced by laser.
JP4634413B2 (en) * 2007-04-23 2011-02-16 テクノシステム株式会社 measuring device

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS58219438A (en) * 1982-06-15 1983-12-20 Kawasaki Steel Corp Spectrochemical analysis device using laser light

Also Published As

Publication number Publication date
JPS6318249A (en) 1988-01-26

Similar Documents

Publication Publication Date Title
EP0781990B1 (en) Raman scattered light measuring apparatus
US2847899A (en) Method of and apparatus for spectrochemical analysis
CA1220643A (en) Method of laser emission spectroscopic analysis of steel and apparatus therefor
US5617205A (en) Spectral measuring method and spectral measuring apparatus
EP0056239A1 (en) Method of measuring Raman spectra and laser Raman spectrophotometry system
Ciucci et al. CF-LIPS: a new approach to LIPS spectra analysis
JP2009288068A (en) Analyzing method and analyzer
KR100326286B1 (en) Isotope analysis process by optical emission spectroscopy on laser-generated plasma
JPH0252980B2 (en)
CN111829971A (en) Method for reducing measurement error of wide spectrum transmittance
JPH06100544B2 (en) Laser emission spectroscopy analyzer
JPH0595035A (en) Analyzer
JPS6394136A (en) Method and instrument for fluorometric analysis
JPS6312527B2 (en)
JP2002005835A (en) Raman spectroscopic measuring apparatus and analytical method for living body sample using the same
JP3660938B2 (en) Component analysis method using laser
JPH112604A (en) Method and device for analyzing element
JPS62188919A (en) Method and instrument for direct emission analysis by multistage laser excitation
JP2006300808A (en) Raman spectrometry system
JPH01112122A (en) Extremely weak light spectroscopic device
JP2000275172A (en) Atomic absorption analysis method and apparatus
JPH0560691A (en) Laser emission spectral analysis method
KR20030054084A (en) Method of laser-induced plasma atomic emission spectroscopy and apparatus thereof
JP2006300671A (en) Spectroscopic detector
JPH09281044A (en) Analytical method for metal carbide

Legal Events

Date Code Title Description
LAPS Cancellation because of no payment of annual fees