Experimental generation of intrinsic localized modes in electrical lattices Lars Q. English...

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xperimental generation of intrinsic localized modes in electrical lattices Lars Q. English Department of Physics & Astronomy Dickinson College, Carlisle, PA (movie: 268 kHz driver frequency) LENCOS 2009, Seville, Spain

Transcript of Experimental generation of intrinsic localized modes in electrical lattices Lars Q. English...

Page 1: Experimental generation of intrinsic localized modes in electrical lattices Lars Q. English Department of Physics & Astronomy Dickinson College, Carlisle,

Experimental generation of intrinsic localized modes in electrical lattices

Lars Q. EnglishDepartment of Physics & Astronomy

Dickinson College, Carlisle, PA

(movie: 268 kHz driver frequency)

LENCOS 2009, Seville, Spain

Page 2: Experimental generation of intrinsic localized modes in electrical lattices Lars Q. English Department of Physics & Astronomy Dickinson College, Carlisle,

Macroscopic lattices Experiments on electrical transmission line

1 unit cell

Fast 24-channel digitizer(now 32 channels)

Lattice

Page 3: Experimental generation of intrinsic localized modes in electrical lattices Lars Q. English Department of Physics & Astronomy Dickinson College, Carlisle,

3

031

2

021

0

0

0

0

1

1ln1

)exp(1

)exp()(

Q

Q

Q

Q

Q

Q

Q

QV

VC

Q

VCVC

Energy Localization in a Nonlinear Electrical Lattice The experimental system

Reverse-biased diode

0

100

200

300

400

500

600

0 2 4 6 8 10

Voltage [V]

Cap

acit

an

ce [

pF

]

np

Charge density

x

21

00 )(

1

V

dd

Page 4: Experimental generation of intrinsic localized modes in electrical lattices Lars Q. English Department of Physics & Astronomy Dickinson College, Carlisle,

.1

11

23

22

2

32

2

000

31

31

320

21

21

21

2

0

21

1121

320

202

0

202

02

2

dt

dV

Rdt

dQ

Q

Q

Q

Q

RC

QQQQ

QQQQ

QQQ

QQ

QQ

Qdt

Qd

dnnn

nnn

nnn

nnn

nnnn

CL20 1 1 11 CL 00 CQ

Duffing Oscillators

Spatially uniformdriving term

Inter-site nonlinearity

NN - coupling

Energy Localization in a Nonlinear Electrical Lattice

Soft-nonlinearity:Quadratic term dominates

cubic term

Uniform mode coupled to uniformMode (k=0)

Linear dispersioncurve; no driver/damping ILM

540 kHz

320 kHz

Page 5: Experimental generation of intrinsic localized modes in electrical lattices Lars Q. English Department of Physics & Astronomy Dickinson College, Carlisle,

Energy Localization in a Nonlinear Electrical Lattice Observation of Discrete breathers /ILMs

fd=300 kHzA=1.5V

fd=268 kHz

Page 6: Experimental generation of intrinsic localized modes in electrical lattices Lars Q. English Department of Physics & Astronomy Dickinson College, Carlisle,

Energy Localization in a Nonlinear Electrical Lattice Parametric excitation / stabilization of ILMs

Red: Node 13Blue: Node 17Black: Node 19

fd=590 kHzA=4.5V

Page 7: Experimental generation of intrinsic localized modes in electrical lattices Lars Q. English Department of Physics & Astronomy Dickinson College, Carlisle,

Energy Localization in a Nonlinear Electrical Lattice Slight change in experimental system

One Unit Cell

Page 8: Experimental generation of intrinsic localized modes in electrical lattices Lars Q. English Department of Physics & Astronomy Dickinson College, Carlisle,

Observation of Traveling ILMs

Energy Localization in a Nonlinear Electrical Lattice

Response to uniform driving below the dispersion curve

Page 9: Experimental generation of intrinsic localized modes in electrical lattices Lars Q. English Department of Physics & Astronomy Dickinson College, Carlisle,

Energy Localization in a Nonlinear Electrical Lattice

Page 10: Experimental generation of intrinsic localized modes in electrical lattices Lars Q. English Department of Physics & Astronomy Dickinson College, Carlisle,

Energy Localization in a Nonlinear Electrical Lattice

Modulational Instability

Incoherent Localized Structures

Coherent structure locked to driver

Patterns of Traveling ILMs

Page 11: Experimental generation of intrinsic localized modes in electrical lattices Lars Q. English Department of Physics & Astronomy Dickinson College, Carlisle,

Energy Localization in a Nonlinear Electrical Lattice

3 ILMs 4 ILMs

3 ILMs 6 ILMs

464 kHz 484 kHz

464 kHz 502 kHz

Patterns of Traveling ILMs

Page 12: Experimental generation of intrinsic localized modes in electrical lattices Lars Q. English Department of Physics & Astronomy Dickinson College, Carlisle,

Energy Localization in a Nonlinear Electrical Lattice

Driver frequency in between regions of integer-number of ILM(here between 3 and 4 ILMs)

Patterns of Traveling ILMs

(472 kHz) (475 kHz)

Page 13: Experimental generation of intrinsic localized modes in electrical lattices Lars Q. English Department of Physics & Astronomy Dickinson College, Carlisle,

Energy Localization in a Nonlinear Electrical Lattice

386 kHz

Switching in a blocking capacitor

cap turned on

Page 14: Experimental generation of intrinsic localized modes in electrical lattices Lars Q. English Department of Physics & Astronomy Dickinson College, Carlisle,

Experiments on 2D macroscopic lattice

Preliminary results: We believe we have observed 2D localization

Energy Localization in a Nonlinear Electrical Lattice

Page 15: Experimental generation of intrinsic localized modes in electrical lattices Lars Q. English Department of Physics & Astronomy Dickinson College, Carlisle,

Energy Localization in a Nonlinear Electrical Lattice

ILM

Preliminary 2d-lattice data

Node

N

ode

Page 16: Experimental generation of intrinsic localized modes in electrical lattices Lars Q. English Department of Physics & Astronomy Dickinson College, Carlisle,

Energy Localization in a Nonlinear Electrical Lattice

Conclusions

• Demonstrated the existence of ILMs/discrete breathers in an electrical lattice

• Fast, multichannel electronic data acquisition makes possible a detailed study of ILM profile and behavior (not possible in other systems)

• Both stationary and slow-moving ILM can be excited in these lattices (depending on the detailed electronic make-up of the unit-cell )

• These ILMs can be generated via modulational instability, parametric instability, or by briefly switching in an impurity.

• Multiple localized features, multi-pulses, can be locked to the driver at higher driver frequencies.