Leica SP8 X Laser Scanning Confocal MicroscopeLeica SP8 X Laser Scanning Confocal Microscope at the...

1
Leica SP8 X Laser Scanning Confocal Microscope at the Advanced Microscopy and Imaging Center University of Tennessee, Knoxville John Dunlap, PhD, Manager FEATURES Spectral Detection a prism (1) splits fluorescence emission sliders (2) define which wavelengths reach different detectors (3) can detect up to five different fluorophores at the same time higher sensitivity with hybrid detctors (HyD) White Light Laser any wavelength from 470 to 670 nm up to 8 simultaneous laser lines pulsed laser (for LightGate) near UV (405 nm) also available argon laser (458, 488, 496, 514 nm) also available LightGate reject photon based on fluorescence lifetime eliminate reflections block autofluorescence collect more signal Resonant Scanner fast scanning of 8,000 lines per second up to 16,000 lines per second with bidirectional scanning for highly dynamic events reduced bleaching of fluorophores Optical Scan Field Rotation adjust scan direction to cell smaller scan area required Fluorescence Recover After Photobleaching (FRAP) for measuring protein dynamics in living cells diffusion constants, turnover rates software wizard for easy setup and analysis Fluorescence Resonance Energy Transfer (FRET) for detecting protein-protein interactions sensitive to changes in distances < 10 nm acceptor bleaching method sensitized emission method software wizard for easy setup 10 µm Organelle Movement in Plant Cells CFP YFP mCherry 50 45 40 35 30 25 20 15 10 5 0 400 500 600 700 800 900 wavelength (nm) HyD Multialkali PMT QE (%) peroxisomes mitochondria Golgi stacks peroxisomes mitochondria Golgi stacks simultaneous image capture with HyD detectors resonant scanner, bidirectional scanning 76 ms per frame 7 focal planes 0.5 µm apart (maximum intensity projection) 547 ms delay between Z stacks kymographs showing all organelles in cell: 10 s LightGate on off Fig. 8 FRAP experiment with FRAP Booster and with FRAP Zoomer. The red line indicates the bleach interval. interval sec Donor Acceptor S1 S1 In the event of FRET an excited fluorophore transfers its energy to another light-absorbing molecule. Split View of 3D Image Stack Protein Localization Inside Chloroplast White Light Laser at 488 nm ISE2-GFP foci (HyD detector 494 – 558 nm) chlorophyll autofluorescence (HyD detector 649 – 725 nm) maximum intensity projection xy view z position at blue line in right image yz view x position at green line in left image plasmodesma-GFP marker (HyD detector 494 – 558 nm) chlorophyll autofluorescence (HyD detector 649 – 725 nm)

Transcript of Leica SP8 X Laser Scanning Confocal MicroscopeLeica SP8 X Laser Scanning Confocal Microscope at the...

Leica SP8 X Laser Scanning Confocal Microscopeat the Advanced Microscopy and Imaging Center

University of Tennessee, KnoxvilleJohn Dunlap, PhD, Manager

FEATURES

Spectral Detection

• a prism (1) splits fluorescence emission

• sliders (2) define which wavelengths reach different detectors (3)

• can detect up to five different fluorophores at the same time

• higher sensitivity with hybrid detctors (HyD)

White Light Laser

• any wavelength from 470 to 670 nm• up to 8 simultaneous laser lines• pulsed laser (for LightGate)• near UV (405 nm) also available• argon laser (458, 488, 496, 514

nm) also available

LightGate

• reject photon based on fluorescence lifetime• eliminate reflections• block autofluorescence• collect more signal

Resonant Scanner

• fast scanning of 8,000 lines per second• up to 16,000 lines per second with

bidirectional scanning• for highly dynamic events• reduced bleaching of fluorophores

Optical Scan Field Rotation

• adjust scan direction to cell• smaller scan area required

Fluorescence Recover After Photobleaching (FRAP)

• for measuring protein dynamics in living cells

• diffusion constants, turnover rates• software wizard for easy setup and

analysis

Fluorescence Resonance Energy Transfer (FRET)

• for detecting protein-protein interactions

• sensitive to changes in distances < 10 nm

• acceptor bleaching method• sensitized emission method• software wizard for easy setup

10 µm

Organelle Movement in Plant Cells

CFPYFPmCherry

50

45

40

35

30

25

20

15

10

5

0

400 500 600 700 800 900

wavelength (nm)

GaAsP PMT

HyD

QE (%

)

50

45

40

35

30

25

20

15

10

5

0

400 500 600 700 800 900

wavelength (nm)

HyD

Multialkali PMT

QE (%

)

Time of flight dispersion in PMTs

Short transit time spread in HyD

Low light intensity High light intensity

Emitted photons

Rapid detector5 counted events

Slow detector3 counted events

http://www.leica-microsystems.com/hyd-guide-qr/

CONNECT WITH US

LEICA HYD'S QUANTUM EFFICIENCY IS SUPERIOR TO STANDARD PMTS AND GaAsP PMTS

Quantum efficiency is a measure for a detector’s capability

to translate photons into electrons. With a typical quantum

efficiency of 45% at 500 nm, the hybrid detector is two to

three times more sensitive than a standard PMT. This new

level of sensitivity improves low-light applications where

traditional PMT-based confocals would fail, such as imaging

of yeast or C. elegans.

Traditional PMTs using a GaAsP (Gallium-Arsenide-Phosphide)

photocathode are susceptible to damage by overexposure.

The Leica HyD’s design avoids this shortcoming, making

the detector both highly sensitive and versatile with a large

dynamic range. In terms of quantum efficiency the Leica HyD

even supersedes standard GaAsP PMTs by delivering

outstanding sensitivity along with durability..

peroxisomes

mitochondria

Golgi stacks

peroxisomesmitochondriaGolgi stacks

simultaneous image capture with HyD detectorsresonant scanner, bidirectional scanning76 ms per frame7 focal planes 0.5 µm apart (maximum intensity projection)547 ms delay between Z stacks

kymographs showing all organelles in cell:

10 s

18

No gating

With gating

λ (nm)

Gain

by

Ligh

tGat

e

The LightGate –Filter Free Removal of Unwanted SignalIn conventional microscopy, reflected and backscattered light is removed by spectral

blocking filters. Leica HyD detectors together with the White Light Laser as a pulsed

excitation source allow the restriction of detection to a certain time gate after the detec-

tion pulse. This removes unwanted signal in an ingeniously simple way.

LIGHTGATE FOR MAXIMUM IMAGE CONTRAST

LightGate utilizes the time decay of the fluorescence signal.

A light pulse from the White Light Laser (WLL) excites the

fluorophores and triggers the start point for time measurement.

Only signals arriving at the hybrid detector in a flexible and

adjustable time window are collected. Unwanted signal from

autofluorescence, backscattered light at the begin of the

fluorescent decay, or detector noise at the end of decay

can be removed. This way, the highest image contrast can

be obtained – even from weakly stained samples.

LightGate onoff

LightGate allows direct detection underneath the laser line to collect more data.

LightGate completely removes cover glass reflection. HeLa cells, nucleus stained with Chromeo 505. Excitation: 510 nm (within detection range). Detection: 495-540 nm

Leica TCS SP8 X –The Only Freely Tunable Confocal SystemThe white light laser source of the Leica TCS SP8 X perfectlymatches the spectral properties of any fluorophore excitable inthe visible spectral range. Continuously tunable excitation and detection ensure best image quality and sample protection. Up to eight excitation lines can be used – simultaneously.

› Tuning range of 470 to 670 nm in 1 nm intervals

› Minimum cross-talk in multiple stained specimen

› Change of Illumination regimes within microseconds

› Lambda Square Mapping: full spectral information by excitation-

emission correlation

› LightGate: background quenching using time-gated detection

› True FLIM results by adjustable excitation wavelength and variable

pulse repetition rate

www.leica-microsystems.com

Cells expressing a cell cycle stage marker. Green: non-S1 phase. Red: S1 phase. Courtesy of Dr. Malte Wachsmuth and Dr. Lars Hufnagel, EMBL,Heidelberg, Germany

Non-S1 phase

S1 phase

Fig. 5 Left: without FRAP Booster. Right: with FRAP Booster. The same laser settings were used for both images . GFP-Tubulin in HeLa cells, EMBL Heidelberg.

5reSOLUTION – FRAP WITH TCS SP8 RESONANT SCANNER

Fig. 6 FRAP experiment without FRAP Booster, without FRAP Zoomer. The red line indicates the bleach pulse.

Fig. 7 FRAP experiment without FRAP Booster, with FRAP Zoomer. The red line indicates the bleach interval

Fig. 8 FRAP experiment with FRAP Booster and with FRAP Zoomer. The red line indicates the bleach interval.

sec

sec

inte

rval

sec

inte

rval

inte

rval

Fig. 6 to 8 is showing the results of FRAP experiments with the resonant scanner.

Fig. 6 Without FRAP booster, without FRAP ZoomerFig. 7 Without FRAP booster, with FRAP ZoomerFig. 8 With FRAP Booster and with FRAP Zoomer

HeLa cells with free YFP were used for the experiments. The FRAP series were taken with a 40x 1.1 lens and zoom factor of 8 was used during the whole ex-periment. The frame rate was about 36 fps, the bleaching time about 200 msec. If you need to bleach even faster, you may use all Ar-laser lines for bleaching.

It can be summarized that during FRAP experiments with RS it may happen that the time to apply the needed laser power is too short to bleach the region of interest efficiently. Then appropriate adjustments are needed to concentrate the available amount of light to a smaller area: The best bleaching results can be achieved by combining the FRAP Zoomer and the FRAP Booster.

2 resolution

F R E T W I T H T C S S P 8

Donor

Acceptor

S1

S1

FRET with Leica TCS SP8 LAS AF

In the event of FRET an excited fluorophore transfers its energy to another light-absorbing molecule.

IntroductionFluorescence Resonance Energy Transfer (FRET) is a tech-nique which allows insights into interactions between pro-teins or molecules in proximities beyond light microscopic resolution. The principle: An excited fluorophore, called donor, transfers its excited state energy to a light-absorbing molecule which is called acceptor. This transfer of energy is non-radiative.

FRET Acceptor PhotobleachingThe method

In the event of FRET the donor encounters a quenching of fluorescence due to its energy transfer to the acceptor. The donor fluorescence will be unquenched after photo-bleaching of the acceptor. The difference in the intensity of the donor before and after photobleaching gives a direct

indication of the FRET efficiency and can be quantified as follows:

FRETeff = (Dpost - Dpre) / Dpost

where Dpost is the fluorescence intensity of the donor after photobleaching and Dpre is the fluorescence intensity of the donor before photobleaching.

Acceptor photobleaching is an established method for the evaluation of FRET efficiencies. It is usually applied to fixed samples, as any relocation of donor molecules during measurement will lead to false intensity correlations.

Split View of 3D Image Stack

Protein Localization Inside Chloroplast

White Light Laser at 488 nmISE2-GFP foci (HyD detector 494 – 558 nm)chlorophyll autofluorescence (HyD detector 649 – 725 nm)maximum intensity projection

xy viewz position at blue line in right image

yz viewx position at green line in left image

plasmodesma-GFP marker (HyD detector 494 – 558 nm)chlorophyll autofluorescence (HyD detector 649 – 725 nm)