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TGPLS MatriX-1
Ultrafast Spectroscopy超快光譜儀
TGPLS MatriX-1 [Time-Resolved Photoluminescence spectroscopy] is the first commercially available broadband fluorescence spectrometer designed for femtosecond amplifier laser systems. Time-resolved fluorescence (or photoluminescenc e) spectroscopy is widely used to reveal electronic excited state dynamics in emissive materials ranging from semiconductors, to nanomaterials, dyes, and proteins. Other time resolved fluorescence spectrometers fall in two categories; broadband spectral resolution with time resolution limited to tens of picoseconds or longer; or ultrafast time resolution limited to single wavelength scans. Neither of these approaches adequately captures ultrafast spectral evolution associated with a host of critical photophysical processes. TGPLS MatriX-1 breaks this tradeoff with the unique ability to capture broadband fluorescence spectra on femtosecond timescales, with high signal quality, low background noise, and rapid data acquisition. The TGPLS MatriX-1 instrument is based on patented transient grating gate technology developed by ultrafast spectroscopy researchers at Victoria University of Wellington, New Zealand. Combining the intrinsic advantages of transient grating gate, and hardware and software user interfaces developed by spectroscopists, TGPLS MatriX-1 is the benchmark next generation time resolved fluorimeter.
TGPLS MatriX-1 [時(shí)間分辨光致發(fā)光光譜儀],是**臺商用的設(shè)計(jì)用于飛秒放大激光系統(tǒng)的寬帶熒光光譜儀。時(shí)間分辨熒光(或光致發(fā)光)光譜廣泛用于揭示發(fā)射材料中的電子激發(fā)態(tài)動力學(xué),從半導(dǎo)體到納米材料、染料和蛋白質(zhì)。其他時(shí)間分辨熒光光譜儀可分為兩類:寬帶光譜分辨率,時(shí)間分辨率限制在幾十皮秒或更長;超快時(shí)間分辨率,僅限于單波長掃描。這兩種方法都不能充分捕捉到與許多關(guān)鍵光物理過程相關(guān)的超快光譜演化。TGPLS MatriX-1 打破了這一局限,它具有捕捉飛秒級寬帶熒光光譜的獨(dú)特能力,具有高信號質(zhì)量、低背景噪聲和高速數(shù)據(jù)采集。TGPLS MatriX-1 是基于由新西蘭惠靈頓維多利亞大學(xué)(Victoria University of Wellington, New Zealand)的超快光譜研究人員開發(fā)的瞬態(tài)光柵**技術(shù)。結(jié)合瞬態(tài)光柵的固有優(yōu)勢,以及光譜儀開發(fā)的軟硬件用戶界面,TGPLS MatriX-1 是下一代時(shí)間分辨熒光計(jì)的基準(zhǔn)。
-Wavelength range: 350 - 750 nm and 850-1300 or 350 - 950 nm and 1050 - 1400 nm 1
波長范圍:350-750mm和850-1300nm,或350-950nm和1050-1400nm 1
-Wavelength resolution: depends on polychrometer
波長分辨率:取決于多色儀
-Delay range: user defined, 600 ps, 1 ns
延遲范圍:用戶自定義,600ps,1ns
-Time resolution: <200 fs based on 100 fs laser source 2
時(shí)間分辨率:<200fs(基于100fs激光源)2
-laser source: femtosecond amplifier, Ti-sapphire or Fiber or Yb:KGW
激光源:飛秒放大器、Ti-Sapphire、光纖或YB:KGW激光器
-Polychrometer: image spectrometer+CCD or monochrometer+PMT
多色儀:圖像光譜儀+CCD或單色儀+PMT
-Dimensions:600 × 900 × 250mm
尺寸:600×900×250mm
1.For Ti-sapphire laser system: 350 – 750 nm and 850-1300. Fiber and Yb:KGW laser system: or 350 – 950 nm and 1050– 1400 nm. The wavelength range also depends on the detectors
對于鈦藍(lán)寶石(Ti-sapphire)激光系統(tǒng):350-750nm和850-1300nm;光纖或Yb:KGW激光系統(tǒng):350-950nm和1050-1400nm。波長范圍也取決于探測器
2.Time resolution depends on the pulse width of the laser source and response time of the gate medium
時(shí)間分辨率取決于激光源的脈沖寬度和門介質(zhì)的反應(yīng)時(shí)間
The TGPLS MatriX-1 is the only spectrometer in the market that allows users to capture broadband fluorescence spectra on femtosecond timescales. The TGPLS MatriX-1 enables users to rapidly acquire high quality spectral data, reduce time spent on cleaning noisy data and integrate into existing spectroscopic workflows. Specifically:
TGPLS Matrix-1是市場上**能夠在飛秒時(shí)間尺度上捕獲寬帶熒光光譜的光譜儀,它使用戶能夠快速獲取高質(zhì)量的光譜數(shù)據(jù),減少清理噪聲數(shù)據(jù)所花費(fèi)的時(shí)間,并容易集成到現(xiàn)有的光譜工作系統(tǒng)中。
特別是:
1.Rapid spectral data acquisition
快速光譜數(shù)據(jù)采集
?Full fluorescence spectral dynamics on sub picosecond timescales (not just kinetics of a single wavelength)
亞皮秒級的全熒光光譜動力學(xué)(不僅僅是單個(gè)波長的動力學(xué))
?Tunable ultrafast gate time window (<200 fs to <1 ps)*
可調(diào)超快快門時(shí)間窗口(<200 fs 到<1 ps)*
?Single high spectral resolution transient spectrum in <2 seconds (with high repetition rate laser source)
<2秒內(nèi)的單一的高光譜分辨率瞬態(tài)光譜(高重復(fù)率激光源)
?Near UV to near IR fluorescence range, compatible with high efficiency photon detectors and high-quality optics in this spectral region
近紫外到近紅外的熒光范圍,在這個(gè)光譜區(qū)域與高效率的光子探測器和高質(zhì)量的光學(xué)兼容
2.High-quality scientific data
高質(zhì)量的科學(xué)數(shù)據(jù)
?Minimal dispersion and aberration with aspherical reflective optics
非球面反射鏡片,具有*小的色散和像差
?Intuitive and repeatable alignment procedure to minimize impact on data noise
直觀和可重復(fù)的校準(zhǔn)程序,以盡量減少對數(shù)據(jù)噪聲的影響
?High quality signals with low excitation intensity (
高質(zhì)量信號,低激勵(lì)強(qiáng)度(
3.Ease of integration
易于集成
?Easy and fast spectral calibration
簡單快速的光譜校準(zhǔn)
?Easy-to-use data acquisition software for automated measurement
簡單易用的可自動測量的數(shù)據(jù)采集軟件
?Ready to be implemented with various ultrafast laser sources: Ti-sapphire, Fiber, Yb:KGW
可用于各種超快激光源:鈦藍(lán)寶石、光纖、Yb:KGW
?Broadband ultrafast spectral evolution selectively probes electronic excited state dynamics and complementary information to other ultrafast spectroscopy techniques
寬帶超快光譜演化選擇性地探測電子激發(fā)態(tài)動力學(xué)和與其他超快光譜技術(shù)的互補(bǔ)信息
* Time resolution depends on the pulse width of the laser source and response time of the gate medium
時(shí)間分辨率取決于激光源的脈沖寬度和柵極介質(zhì)的響應(yīng)時(shí)間
Fig.1.The scheme of TGPLS MatriX-1
圖1. TGPLS MatriX-1原理示意圖
Ultrafast photo-excitation dynamics inoptoelectronic materials
光電材料中的超快光激發(fā)動力學(xué)
Ultrafast PL spectral evolution reveals charge and excitondynamics in advanced optoelectronic materials.
超快PL光譜演化揭示了先進(jìn)光電材料中的電荷和激子動力學(xué)
Fig. 2. The spectral contours of CH3NH3PbI3 thin film(a) 1 uJ/cm2, (b) 3 uJ/cm2, (c) 6 uJ/cm2, and (d)15 uJ/cm2.The ultrafast carrier cooling processes can be directlyinvestigated by the dynamics of carrier temperatureextracted from TRPL spectrum.
圖2. CH3NH3PbI3薄膜的光譜輪廓(a) 1 μJ/cm2,(b) 3 μJ /cm2,(c) 6 μJ /cm2,(d)15 μJ /cm2。利用TRPL譜中載流子溫度的動態(tài)變化可以直接研究超高速載流子冷卻過程
Ultrafast energy transfer(d)
超快能量轉(zhuǎn)移
Intramolecular resonance energy transfer in multichromophore arrays is studied by TGPLS.
利用TGPLS研究多色團(tuán)陣列的分子內(nèi)共振能量轉(zhuǎn)移
Fig. 3. (a) TRPL spectra of dimer (b) kinetics of the donorand acceptor
圖3. (a) 二聚體的TRPL譜,(b) 供體和受體的動力學(xué)
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