single-molecule methods i - in · pdf filebrief history of single molecule methods •1989...
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Single-Molecule Methods I - in vitro
Bo Huang
Macromolecules
2013.03.11
F1-ATPase: a case study
ADP ATP
Membrane
Rotation of the axle when hydrolyzing ATP
Kinosita group, 1997-2005
Single Molecule Methods
Noji group, 2005
Why look at molecules, one at a time?
An ensemble picture
Single Object Measurement: Resolving Heterogeneities
Most people are eating... But some are cooking
Single Object Measurement: Resolving Heterogeneities
Conformation states of protein folding
Laurance, Kong, Jager and Weiss, PNAS, 2005 (102), p 17348
Single Object Measurement: Avoiding Synchronization
Single object movies
Myosin walk on actin filament
F1 – ATPase rotation
Single Object Measurement: Avoiding Synchronization
1
2
3
Single Object Measurement: Detecting Rare Species
Single Object Measurement: Detecting Rare Species
RNA polymerase at work
Backtracking (0.1% probability) to correct for base pair mismatch
Abbondanzieri, Greenleaf, Shaevitz, Landick and Block., Nature 2005 (438), p 460
Brief history of single molecule methods
• 1989 - W.E. Moerner - Absorption
• 1990 - M. Oritt - Fluorescence
• 1993 - Room temperature (NSOM)
• 1994 - Confocal
• 1995 - TIRF
• 1998 - Optical trap
• 1996-2001 Single pair FRET
• 2003 - Single molecule localization
• 2000-2006 - Super-resolution microscopy
Single-Molecule Experiments
Fluorescence Force
Pulling a Molecule
• Atomic force microscope
• Optical trap
• Magnetic tweezers
• Buffer flow
Protein Unfolding by AFM
Optical trap
Magnetic Tweezers
Flow-stretching
Labeled DNA (free) Labeled DNA (flow) DNA+nucleosome (flow)
How to detect single molecule fluorescence?
• Great fluorophores
• Low background
• Sensitive detection
• Single molecule concentration
Lavis & Raines, ACS Chem Biol, 2008
“Good” Organic Fluorophores
Reducing background: confocal
Plan Apo 100x Oil NA 1.4
APD or PMT
Reducing background: TIRF
CCD
Sensitive detection
High NA Objective $5,000 ~ $15,000
EMCCD $20,000 ~ $40,000
APD $3,000 ~ $10,000
Single molecule concentration
0 1 2 3 40.0
0.2
0.4
0.6
0.8
1.0
Pro
ba
bili
ty
Number of molecules0 1 2 3 4
0.0
0.2
0.4
0.6
0.8
1.0
Pro
ba
bili
ty
Number of molecules0 1 2 3 4
0.0
0.2
0.4
0.6
0.8
1.0
Pro
ba
bili
ty
Number of molecules
1 2 3 40.00
0.02
0.04
0.06
0.08
0.10
Navg = 1 Navg = 0.5 Navg = 0.1
The number of molecules in the detection volume follows Poisson distribution
P(k; Navg) = Navgk e-Navg / k! Ensuring single molecule detection
↓ No molecule most of the time!
Single molecule concentration
Confocal detection volume ≈ 1 µm3 = 1 fL
Navg = 1 1/(6 × 1023) mol / 1 × 10-15L ≈ 2 nM
Navg = 0.1 200 pM
Single molecule concentration ≤ 100 pM
TIRF detection volume ≈ 0.1 fL
Navg = 1 20 nM
“Few molecule” spectroscopy
0 500 1000 1500 2000 2500 3000 3500 4000 4500 50000
100
200
300
400
500
600
Co
un
ts
Time / us
1.5
1.4
1.3
1.2
1.1
1.0
10 -6
10 -5
10 -4
10 -3
10 -2
10 -1
10 0
Fluorescence correlation spectroscopy (FCS)
Autocorrelation
1/C
on
cen
trat
ion
Diffusion time
The simplest single molecule experiment: Fluorophore counting
Ulbrich & Isacoff, Nat Methods, 2007
Single-pair FRET
Fluorescence Resonance Energy Transfer (FRET)
Donor
Acceptor
FRET efficiency: Quantum efficiency of energy transfer
E = kFRET / (kFRET + kfl + knr)
Often approximated by “proximity ratio”
E ≈ Iacceptor / (Idonor + Iacceptor)
Fluorescence
Nonradioactive decay
kfl
knr
kFRET
Energy transfer
FRET efficiency
Donor
Acceptor
R
6
0
1
1
R
RE
0 1 2 0
0.5
1
E
R/R0
Förster Radius
R06 = 8.8 × 1023 κ2 n-4 Q0 J
Orientation factor (0 ≤ κ ≤ 4) usually 2/3 (caution!)
Refractive index
Donor quantum efficiency
Overlap integral J = ∫ fD(λ) εA(λ) λ4 dλ
The Förster radius can be calculated from measurable parameters
For common FRET pairs, R0 ≈ 4-6 nm
Donor emission Accepter absorption
Diffusion spFRET
FRET efficiency
Immobilized spFRET
What can we measure?
T. Ha Group
FRET histogram
Time
Dwell time distribution FRET transition matrix
Typical spFRET setup
Total internal reflection fluorescence microscopy
θ1 = 90°
sinθ2 ≡ sinθc = n1/n2
n1
n2
θ1
θ2
n1sinθ1 = n2sinθ2
Total internal reflection:
n1 = 1.33 (water), n2 = 1.52 (glass), θc = 61°
The evanescent wave in TIR
• The energy of the evanescent wave is localized near the interface.
• The strength of the evanescent wave field decreases exponentially.
• The penetration depth is a function of the wavelength and the incident angle.
• Typical penetration depth: 50-100 nm.
TIRM improves S/N for surface imaging
Epifluorescence TIRF
Prism-type TIRF configuration
CCD
Quartz slide
Spacer Buffer
Coverglass
Through-the-objective TIRF
Requirement for TIRF objective
NA = nglass sinθmax
nwater = nglass sinθc
θmax ≥ θc
NA ≥ nwater ≈ 1.33
TIRF compatible objectives
• 1.40 NA – “Barely enough” for laser TIRF
• 1.45 / 1.49 NA “TIRF” objective – More homogenous illumination field
– Higher efficiency for lamp TIRF
– Compromised image quality
• 1.65 NA – Sapphire coverglass
– Toxic oil…
Prism vs. Objective type TIRF
Prism
• More complicated illumination
• Water immersion objective
• Quartz slides
• High S/N
Objective
• Simple setup
• Oil immersion objective
• Ordinary coverglass
• Higher signal but even higher background
Surface Immobilization
Streptavidin Neutravidin
Streptavidin Neutravidin
Biotinylated lipid
The classic flow channel
The Full Jabłonski Diagram
hν
hν
Emission
Intersystem crossing
Triplet State
Vibration relaxation
hν
Phosphorescence Triplet
Quenching
Lifetime ≈ μs - ms
Absorption
S1
S0
T1
Non-radioactive decay
Photobleaching
hν
Absorption
Triplet State
Vibration relaxation Intersystem crossing
Most common cause: O2
S1
S0
T1
Fight against photobleaching
Donor photobleaching
The oxygen scavenging system
Glucose + O2
Glucose oxidase
Gluconic acid + H2O2
Catalase
H2O
2 ×
Triplet quencher:
β-mercaptoethanol
β-mercaptoethylamine
HO-CH2-CH2-SH
H3N-CH2-CH2-SH
Trolox
Alternated Excitation (ALEX)
Analysis
Coming up:
Single-molecule methods in cells