4
GEMINI an ultra-stable interferometer • High throughput that allows high sensitivities • ≈1 attosecond stability between the two replicas of light • Fast scans (<1 sec.) • Scan range selectable by the user • Compact and low-cost • Insensitive to vibrations • Interferometry • Generation of pulse pairs GEMINI IN DETECTION PATH • Time- and frequency- resolved fluorescence • Pump-probe spectroscopy • Coherent Raman spectroscopy GEMINI IN EXCITATION PATH • Fluorescence Excitation-Emission Maps • Characterization of single molecules GEMINI is a novel and compact interferometer that can guarantee very high robustness and stability between the two generated replicas of light. The exceptional performances of this device can be exploited in many different applications, such as time- and frequency-resolved fluorescence, coherent Raman, pump-probe, two-dimensional spectroscopy and studies on single molecules. Key Features Applications

GEMINI Brochure version 3 - nireos.com · 650 700 750 800 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 Time (ns) Wavelength (nm) Intensity Intensity (a.u.) (a.u.)-1 0 1 2 3 4 5 6 7 8 9

  • Upload
    others

  • View
    2

  • Download
    0

Embed Size (px)

Citation preview

Page 1: GEMINI Brochure version 3 - nireos.com · 650 700 750 800 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 Time (ns) Wavelength (nm) Intensity Intensity (a.u.) (a.u.)-1 0 1 2 3 4 5 6 7 8 9

GEMINI an ultra-stable interferometer

• High throughput that allows high sensitivities• ≈1 attosecond stability between the two replicas of light • Fast scans (<1 sec.)• Scan range selectable by the user• Compact and low-cost• Insensitive to vibrations

• Interferometry• Generation of pulse pairs

GEMINI IN DETECTION PATH• Time- and frequency- resolved fluorescence• Pump-probe spectroscopy• Coherent Raman spectroscopy

GEMINI IN EXCITATION PATH• Fluorescence Excitation-Emission Maps• Characterization of single molecules

GEMINI is a novel and compact interferometer that can guarantee very high robustness and stability between the two generated replicas of light. The exceptional performances of this device can be exploited in many di�erent applications, such as time- and frequency-resolved �uorescence, coherent Raman, pump-probe, two-dimensional spectroscopy and studies on single molecules.

Key Features Applications

Page 2: GEMINI Brochure version 3 - nireos.com · 650 700 750 800 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 Time (ns) Wavelength (nm) Intensity Intensity (a.u.) (a.u.)-1 0 1 2 3 4 5 6 7 8 9

6

5

0

7

0

0

7

5

0

8

0

0

0

0

.1

0

.2

0

.3

0

.4

0

.5

0

.6

0

.7

0

.8

0

.9

1

Time (ns)

Wav

elen

gth

(nm

)

Intensity(a.u.)In

tens

ity(a

.u.)

-1 0 1 2 3 4 5 6 7 8 90.01

0.1

1

540 580 620 660 700 7400

0.1

0.2

0.3

0.4

0.5

0.6

0.7

0.8

0.9

-1 0 1 2 3 4 5 6 7 8 9500

550

600

650

700

750

800

t=1.8 ns

t=4.2 ns

Time (ns) Time (ns)

Wav

elen

gth

(nm

)

Wavelength (nm)

Wavelength (nm) Wavelength (nm)

Inte

nsity

(a.u

.)

Inte

nsity

(a.u

.)

650

700

750

-1 0 1 2 3 4 5 6 7 8 9

-1 0 1 2 3 4 5 6 7 8 90

0.1

0.2

0.3

0.4

0.5

0.6

0.7

0.8

0.9

1

800

Sam

ple

SPAD orPMT

TCSPC

Time- and frequency-resolved fluorescence with a single TCSPC detector

500 550 600 650 700 750 600550 650 750700

Experimental setup: GEMINI interferometer is placed in collection before the detector (a SPAD or PMT) connected to a TCSPC. This allows one to resolve the �uorescence wavelength axis while preserving the temporal resolution.

Fluorescence maps as a function of detection wavelength and emission time for a mixture of Rhodamine B and Nile Red in acetone solution.

Semi-log plots of �uorescence decay traces at ≈575 nm (green curve) and ≈675 nm (purple curve).

Integrated spectra of the two �uorophores computed from the correspondent Decay Associated Spectra (DAS) and lifetimes.

Rhodamine B + Nile Red

LHCS3R complex

(a) Fluorescence map of the LHCSR3 complex from C. reinhardtii; (b-c) Marginals of (a), obtained by integrat-ing the map along the horizontal and vertical directions, respectively, showing the overall �uorescence spectrum and decay dynamics.

Comparison of �uorescence emission spectra of Rhodamine B, measured in the same experimental conditions. Excitation laser: =530 nm, P=1 W.

(a) (b)

(c)

A. Perri et al., Opt. Express 26, 2270-2279 (2018).

Standard grating-based spectrometer

GEMINI + single PMT detector

00

600550 650 750700

GEMINIInterferometer

The GEMINI can be placed as a turn-key add-on

device

Narrowband pulsed excitation

Page 3: GEMINI Brochure version 3 - nireos.com · 650 700 750 800 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 Time (ns) Wavelength (nm) Intensity Intensity (a.u.) (a.u.)-1 0 1 2 3 4 5 6 7 8 9

SampleBroadbandProbe/Stokes

Modulated

Narrowband Pump

Photo-diode

Lock-inAmpli�er

Experimental setup: GEMINI interferometer is placed in the probe/Stokes beam after the sample, allowing one to measure SRS or pump-probe spectra up to MHz modulation frequencies.

Coherent Raman (Stimulated Raman Scattering - SRS) and Pump-Probe Spectroscopy

1400

1200

1300

1400

Wav

elen

gth

(nm

)

1100

5

-5

(a) Two-dimensional ΔT⁄T(λ,τ) map for a graphite sample prepared by liquid phase exfoliation. (b) ΔT⁄T spectra at selected probe delays; (c) ΔT⁄T dynamics at 1270-nm probe wavelength (red circles) together with a bi-exponential �t (black solid line). Inset: zoom of the signal for negative delays.

(a) (b)

(c)

Chemometric analysis of the acquired dataset. (a) SRS spectra for PMMA (solid black line) and PS (dotted red line). (b) False-color image of the sample, showing a central bead of PMMA (in red), surrounded by smaller beads of PS (in green). (c) and (d): concentrations maps of PMMA and PS.

F. Preda et al., Opt. Lett. 41, 2970-2973 (2016). J. Réhault et al., Opt. Express 23, 25235-25246 (2015).

The GEMINI is designed to be added to your setup to extract the spectrum of any light source, coherent or not. It can replace monochromators, since it overcomes their main drawbacks in terms of low throughput, �xed spectral

resolution and limited spectral coverage

COMPARISON between GEMINI and a monochromator. The �uorescence of a sample is collected at 90° and measured with PMT detectors. The GEMINI and the monochromator enable to spectrally resolve the �uorescence. With the GEMINI, one can obtain the same S/N obtained with a monochromator with ~100 times lower excitation light power.

GEMINIInterferometer

Mon

ochr

omat

or

PMTdetector

PMTdetector

FluorescentSample

ExcitationLaser

GEMINIInterferometer

Comparison with Monochromators

GEMINI

Monochromator

Page 4: GEMINI Brochure version 3 - nireos.com · 650 700 750 800 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 Time (ns) Wavelength (nm) Intensity Intensity (a.u.) (a.u.)-1 0 1 2 3 4 5 6 7 8 9

Speci�cations can be subject to change without notice. For more information, please contact us via e-mail at [email protected] or visit our website www.nireos.com

Excitation-Emission Maps (EEMs) of Single Molecules

GEMINI interferometer allows the characterization

of single molecules with low acquisition times and exceptional accuracy and

sensitivity

Technical SpecificationsVERSION S M L

Spectral range [nm] 250 - 3500

Max. Delay τ [fs @ λ=600 nm] SYM ± 400 ± 700 ± 1050

ASY -100 → 700 -100 → 1300 -100 → 2000

Delay τ Stability < 1 a�osecond

Modes of Opera�on Con�nuous Scan or Step Scan*

Dimensions [mm] 100 x 110 x 65

Weight [kg]

*In step scan mode, the user can select the dwell time for each delay via software

(500 - 4500 on request)

0.4

Broadbandexcitation

Sample

Objective

Long Pass Filter

Beam Splitter

Flip Mirror

Short PassFilter

Photodiode and TCSPC

GEMINIInterferometer

WhiteLight

Source

Spectrograph

The GEMINI can be placed as a turn-key add-on device

0

GEMINI Interferometer Position [mm] Excitation Wavenumber /103 [cm-1]

Det

ectio

n W

aven

umbe

r /10

3 [cm

-1]

Excitation Wavenumber /103 [cm-1]

Dec

ay T

ime

[ns]

Det

ectio

n W

aven

umbe

r /10

3 [cm

-1]

(from

Spe

ctro

grap

h)

FT

GEMINI in ExcitationSpectrograph in Detection

GEMINI in ExcitationPhotodiode+TCSPC in Detection

EXCITATION-EMISSION MAP TIME and FREQUENCY-RESOLVED MAP

Single Molecule interferogram (A) and relative Excitation-Emission Map (B) obtained via Fourier Transform (FT) along the x-axis. (C) Excitation-energy versus emission-intensity decay for a single molecule constructed from an interferometric TCSPC experiment.

A B

C

Thyrhaug et al., “Single-molecule excitation–emission spectroscopy”, PNAS 201808290 (2019).

Single molecule: Terrylene diimide derivative