nanomechanics - capri school · yaroslav m. blanter capri school, april 2016 measurements of...
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Capri School, April 2016Yaroslav M. Blanter
Nanomechanics
Yaroslav M. Blanter
Kavli Institute of Nanoscience, Delft University of Technology
Detection Shuttling Doubly-clamped beams Graphene Strain engineering
Capri School, April 2016Yaroslav M. Blanter
Persistent currents
22
22
20
22
20
ˆ ˆ2
ˆ ;2
( )
2
iN
eH p A
m c
H imR
e
E NmR
f
f
f
æ ö= - Þç ÷è ø
æ ö¶ F= - -ç ÷¶ Fè ø
Y µ Þ
æ öF= -ç ÷Fè ø
r rh
h
h
Interference is affected by Aharomov-Bohm flux
Energy levels vs. flux
RA
0
0-2
2 -2
22
2/
2E
mR
h
Capri School, April 2016Yaroslav M. Blanter
Measurements of persistent currents
A. C. Bleszynski-Jayich et al, Science 326, 272 (2009)
i
filledlevels
EEI
¶¶= =¶F ¶Få
Amplitude clean, single ring:2
e
mR
h
Amplitude disordered:
20
2 4sin ,l l
l
l eI I I
p dp
F= = -
Få h
Difficult to measure!
Capri School, April 2016Yaroslav M. Blanter
A. C. Bleszynski-Jayich et al, Science 326, 272 (2009)
Measurements of persistent currents
Currents produce tork and shiftthe cantilever frequency
Good agreement with the theorypredictions
Bt m= ´
Capri School, April 2016Yaroslav M. Blanter
Mass detection
Y. T. Yang et al (Roukes group, Caltech) Nano Letters 6, 583 (2006)
Resonant frequency: 133 MHzSize: 2300 x 150 x 70 nmMass sensitivity: 100 zg
Capri School, April 2016Yaroslav M. Blanter
M. S. Hanay et al, Nature nanotech. 7, 602 (2012)
Single-molecule detection
Capri School, April 2016Yaroslav M. Blanter
Shuttling
Couples phonons to charge due tothe position dependence of tunnelrates and of Coulomb-induced force
D. R. König and E. M. Weig APL 101, 213111 (2012)
L. Y. Gorelik et al PRL 80, 4526 (1998)
S D
Capri School, April 2016Yaroslav M. Blanter
Double-clamped beam
Couples phonons to charge due tothe Coulomb-induced force
G. Steele et al Science 325, 1103 (2009)
Size: 500 nmFrequency: 140 MHzQ-factor: over
S. Sapmaz et al PRB 67, 235414 (2003)
L R
G
Lz
[ ]C z
510
Capri School, April 2016Yaroslav M. Blanter
Backaction in a double-clamped beam
H. B. Meerwaldt, G. Labadze, B. H. Schneider, A. Taspinar, YMB, H. S. J. van der Zant, and G. A. Steele, PRB 86, 115454 (2012)
200
2 3
cos [ ]
[ ]
RF
MMx x M x F t F x
Q
F x kx x x
ww w
b a
+ + = +
= -D - -
&& &
( )21
2g
g CNT
dCF V V
dx= -
Renormalization of frequency and introducing of Duffing parameter
Capri School, April 2016Yaroslav M. Blanter
Frequency stiffening by Coulomb effects
0 ~ 1 tot
g g g
NC e
C C Vw
¶D µ - -
¶G. Steele et al Science 325, 1103 (2009)
Capri School, April 2016Yaroslav M. Blanter
Coulomb blockade
LV
0RV =
1nS +
nS
Conditions that current is not flowing:
1n LS eV+ >(a)
1 0nS + >(c)
n LS eV<(b)
0nS <(d)GV
V
0n =1n =
Capri School, April 2016Yaroslav M. Blanter
Frequency softening by Coulomb effects
0 ~ 1 tot
g g g
NC e
C C Vw
¶D µ - -
¶
H. B. Meerwaldt et al, PRB 86, 115454 (2012)
Capri School, April 2016Yaroslav M. Blanter
Coulomb-induced nonlinearity
2 3[ ]F x kx x xb a= -D - -
Capri School, April 2016Yaroslav M. Blanter
Coulomb-induced damping
0 0
0
1stoch g g
g tot g
F V dC N
Q Q mC dx V
w w ¶= +
G ¶
O. Usmani, YMB, and Yu. V.Nazarov, PRB 75, 195312 (2007)
Capri School, April 2016Yaroslav M. Blanter
Backaction in SET coupled to a resonator
O. Usmani, YMB, and Yu. V. Nazarov, ‘04, '07
( , , )nP x v t
[ ]nn
P Fv P St P
t x v M
¶ ¶ ¶æ ö+ + =ç ÷¶ ¶ ¶è øAdiabaticity: reduce to Fokker-Planck equation
- obeys master equation x – positionv - velocity
2( , )F x v M x M v Fnw g= - - +
22
2( ) ( ) ( )
P P P Pv x x vP D x
t x v Q v v
ww é ù¶ ¶ ¶ ¶ ¶+ - - + Y =ê ú¶ ¶ ¶ ¶ ¶ë û
Built-in dissipationDissipation due to tunneling Diffusion in
velocity space2
2 3
( ) ( ) ( ) ( )( ) x x
t
x x x xFx
M
- + + -G ¶ G -G ¶ GY =
G
Capri School, April 2016Yaroslav M. Blanter
Coulomb-induced instabilities
0 0
0
1stoch g g
g tot g
F V dC N
Q Q mC dx V
w w ¶= +
G ¶
O. Usmani, Ya. M. Blanter, and Yu. V.Nazarov, PRB 75, 195312 (2007)
, ,( ),
,
2
( ( ))
L R L Ra E FxL R
F L R
e
f E Fx
D +±G =
´ ± D +
Capri School, April 2016Yaroslav M. Blanter
Strain in graphene
Suzuura, Ando ‘02Guinea, Katsnelson, Vozmediano '08
Deformation of a graphene sheet acts at electrons as pseudomagnetic field in the Dirac equation
( ); 2 ; 3x xx yy y xyA t u u A t ub b b= - = - »
Deformation caused by uniform load:
22 204
( )h
h r R rR
Uniform load Local load (center)
( ) ( ) ( )Fv p A r E rs + Y = Yrr r r rDirac equation: with added gauge fields
Deformation caused by local load:
( )2 2 202
1( ) ln
2
h Rh r R r r
R ræ ö= - -ç ÷è ø
R0h
K.-J.Kim, YMB, K.-H.AhnPhys. Rev. B 84, 081401 (2011)
Capri School, April 2016Yaroslav M. Blanter
Piezoconductivity in graphene
Deformation: Creates strain: pseudomagnetic gauge fields Creates density redistribution; the profile needs inprinciple to be calculated self-consistently
Fogler, Guinea, and KatsnelsonPhys. Rev. Lett. 101, 226804 (2008)
Local shift of the Dirac cones:Predicted metal-insulator transition at certaindeformation
Capri School, April 2016Yaroslav M. Blanter
Piezoconductivity in graphene
M. V. Medvedyeva and YMBPhys. Rev. B 83, 045426 (2011)
Capri School, April 2016Yaroslav M. Blanter
Strain engineering in MoS2
A. Castellanos-Gomez et alNano Lett. 13, 5361 (2013)
Wrinkles: large strain difference
Capri School, April 2016Yaroslav M. Blanter
Strain engineering in MoS2
A. Castellanos-Gomez et alNano Lett. 13, 5361 (2013)
Funneling of excitons