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How we can describe the polarizated light from a VCSEL laser?

Jan 03, 2016

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Why we are interested in light? Because photons are the most fast particle in nature which we can control and detect it. By LASER cavities we can generate beams photons light polarized in two orthogonal directions. - PowerPoint PPT Presentation
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Page 1: How we can describe the polarizated light from a VCSEL laser?
Page 2: How we can describe the polarizated light from a VCSEL laser?

How we can describe the polarizated light from a VCSEL laser?

Why we are interested in light?

Because photons are the most fast particle in nature which we can control and detect it.

By LASER cavities we can generate beams photons light polarized in two orthogonal directions.

Quantistic Physical Phenomena appears due to the chaotic and stochastic nature of the system, which generate a bistability in the polarization modes with an histeresis cycle.

Page 3: How we can describe the polarizated light from a VCSEL laser?

EQUATIONS RATE in a Solitary LASER – Current controlled

PARAMETERS DEFINITIONS AND VALUES USED

k Field decay rate 300 ns-1

Linewidth enhancement factor 3

Injection current [1:5]

s Spin-Flip relaxation rate 50 ns-1

a Gain anisotropies - dichroism 0,5 ns-1

p Linear anisotropies - birefringence 50 rad ns-1

N Decay rate total carrier population 1 ns-1

N Total carrier density

n Difference carrier density

sp Coefficient spontaneus emission [1e-6: 1]

Page 4: How we can describe the polarizated light from a VCSEL laser?

Current from 0.9 to 1,3 in 200 ns Current from 0.9 to 1,3 in 25 ns

Characteristic Intensities Modes- Current

Page 5: How we can describe the polarizated light from a VCSEL laser?

Characteristic Intensities Modes- Current

Noise strength=1e-6

Noise strength=1Noise strength=1e-2

Noise strength=1e-4

Page 6: How we can describe the polarizated light from a VCSEL laser?

22 * *

22 * *

1 1 ,

1 1 ,

1 ,

,

xx y a p x sp N x

yy x a p y sp N y inj

N x y y x x y

s N x y y x x y

dEk i N E inE i E N

dtdE

k i N E inE i E N kEdtdN

N E E in E E E Edtdn

n n E E iN E E E Edt

Rate Equations model in Master-Slave configuration

is defined as the difference between and the intermediate Frequency between the two linearly polarized modes of the solitaryVCSEL .

0x y

Page 7: How we can describe the polarizated light from a VCSEL laser?

N

(ns-1)p

(rad ns-1)s

(ns-1)a

(ns-1)

(rad ns-1)Einj sp K

(ns-1)

3 2,5 1 30 50 0,5 12 ----- 1e-5 300

Polarization modes in Master-Slave configurationwith different ramp long scan of the injected power

Page 8: How we can describe the polarizated light from a VCSEL laser?

X-Mode PS encoding OR logic Output increasing Noise strength

Page 9: How we can describe the polarizated light from a VCSEL laser?

Probability of success Logic Operation

Page 10: How we can describe the polarizated light from a VCSEL laser?

Probability maps

Page 11: How we can describe the polarizated light from a VCSEL laser?

Optimal parameters

Page 12: How we can describe the polarizated light from a VCSEL laser?

Conclusions

Page 13: How we can describe the polarizated light from a VCSEL laser?

Thank you for your attention!