Ghost Imaging Ghost Imaging Sean Crosby Sean Crosby Supervisor: Associate Professor Ann Roberts Supervisor: Associate Professor Ann Roberts Optics Annual Talks Optics Annual Talks 8 March 2005 8 March 2005
Dec 19, 2015
Ghost ImagingGhost Imaging
Sean CrosbySean CrosbySupervisor: Associate Professor Ann RobertsSupervisor: Associate Professor Ann Roberts
Optics Annual TalksOptics Annual Talks8 March 20058 March 2005
OutlineOutline
Why do I want to do this?Why do I want to do this? How do I do this?How do I do this? Induction into the Optics groupInduction into the Optics group How to improve it?How to improve it? (Helpful) hints for grasshoppers….(Helpful) hints for grasshoppers….
What brought on the madness?What brought on the madness?
Einstein and his Posse of Rogues (EPR) Einstein and his Posse of Rogues (EPR) thought of entanglementthought of entanglement
Entanglement has become experimentally Entanglement has become experimentally feasible -> no longer just a thoughtfeasible -> no longer just a thought
Entanglement presents us with novel Entanglement presents us with novel relations between individual photonsrelations between individual photons
Lets use them!Lets use them!
50c explanation of entangled 50c explanation of entangled sourcessources
Two photons are created at the same time by Two photons are created at the same time by destroying one incoming photondestroying one incoming photon
All the photons have some relationship between All the photons have some relationship between themthem
Normally this relationship is conservation of Normally this relationship is conservation of momentum and/or energymomentum and/or energy
Magic Media
Properties of entangled sourcesProperties of entangled sources
The two photons are created at the same timeThe two photons are created at the same time So we can be assured that if a photon is in one So we can be assured that if a photon is in one
beam, there is another in the other beam -> beam, there is another in the other beam -> temporal coherence temporal coherence between between the beamsthe beams
Because of momentum conservation, prediction Because of momentum conservation, prediction of position of other photon is possible -> spatial of position of other photon is possible -> spatial coherence coherence betweenbetween the beams the beams
Hang on Giles…….Hang on Giles…….
This sounds expensive, and you need a lot This sounds expensive, and you need a lot of equipment to get this working of equipment to get this working
Magic Media…. Preposterous!Magic Media…. Preposterous! Can’t you do it using stuff the Egyptians Can’t you do it using stuff the Egyptians
could’ve conceived using?could’ve conceived using?
In a word, Yes!In a word, Yes!
Need spatial and temporal coherence between Need spatial and temporal coherence between two beamstwo beams
First things first -> lets create two beams from First things first -> lets create two beams from oneone
Well, how do we create two beams from one?Well, how do we create two beams from one?
Splitting the beam…..Splitting the beam…..
Beam 1
Beam 2
ThermalLight Source
So simply by splitting the beam into two, we have a spatially “entangled” source
Surprise!Surprise!
Even though not concurrently, every photon in one beam “exists” in the other beamSpatial correlations become greater as intensity increases, because photons in time become “squished together” and “overlap”
Where to?Where to?
Lets get imaging……..Lets get imaging…….. Source creates them at the same time -> Source creates them at the same time ->
at least we could do is measure them at at least we could do is measure them at the same timethe same time
Is this coincidental?Is this coincidental?
I sense something spooky….I sense something spooky…. Imaging in coincidence lets us “multiply” Imaging in coincidence lets us “multiply”
the information in the two beams to obtain the information in the two beams to obtain an image -> object doesn’t have to be in an image -> object doesn’t have to be in both beams!both beams!
Signal Beam
DetectorIdler Beam
Object
Detector
That’s a little simplistic….That’s a little simplistic….
We need to “image” the beam onto the We need to “image” the beam onto the detectordetector
Signal Beam
DetectorIdler Beam
Object
Detector
F
2F2F
A World Exclusive….A World Exclusive….
Coincidence
So what’s happening physically?So what’s happening physically?
Signal beam -> each pixel of the detector Signal beam -> each pixel of the detector will have a single spatial frequencywill have a single spatial frequency
Idler beam -> near field image of the beam Idler beam -> near field image of the beam at the conjugate object positionat the conjugate object position
How do we know the multitude of photons How do we know the multitude of photons hitting the detector are correlated with hitting the detector are correlated with each other?each other?
Coincidink…Coincidink…
Image = <I1I2>-<I1><I2>
I feel a little underwhelmed….I feel a little underwhelmed….
So, how do we make the image clearer, or So, how do we make the image clearer, or my favourite, completely wreck it?my favourite, completely wreck it?
Coherence of source!Coherence of source! Increasing the coherence “smears” out the Increasing the coherence “smears” out the
object imageobject image
Delocating…..Delocating…..
Given the position of one photon, Spatial Given the position of one photon, Spatial coherence increases the “uncertainty” in coherence increases the “uncertainty” in the position of the other photonthe position of the other photon
Non-zero quantum probability of the Non-zero quantum probability of the photon being anywhere within predicted photon being anywhere within predicted position +/- coherence length of sourceposition +/- coherence length of source
Lose the ability to absolutely predict where Lose the ability to absolutely predict where the photons are -> decreased correlationsthe photons are -> decreased correlations
On the road to home…On the road to home…
Must quantify this coherence relationship Must quantify this coherence relationship -> My First Paper-> My First Paper
I am still not using my $8000 presents….I am still not using my $8000 presents…. Image something elseImage something else Extend to entanglement?Extend to entanglement? Quantify how the phase of the object Quantify how the phase of the object
affects the intensity measurementaffects the intensity measurement
Things I Have Learnt…Things I Have Learnt…
Make a regular time with your supervisorMake a regular time with your supervisor Do write up as you go Do write up as you go
These talks are much easier to prepareThese talks are much easier to prepare Answers to questions you ask yourself Answers to questions you ask yourself
naturally flow when writingnaturally flow when writing It makes everything link together in your mind It makes everything link together in your mind
-> so much more fun!-> so much more fun!
What is entanglement?What is entanglement?
A non-separability of the multi-particle wavefunction for A non-separability of the multi-particle wavefunction for 1 or more observables1 or more observables
In the two entangled object case, if we measure one In the two entangled object case, if we measure one property (energy, momentum, polarisation) of one of property (energy, momentum, polarisation) of one of the entangled objects, we can predict the SAME the entangled objects, we can predict the SAME property of the other entangled object with absolute property of the other entangled object with absolute certaintycertainty
)(),...,,( 21 nnn xxxx
How is it experimentally prepared?How is it experimentally prepared?
Entanglement is analogous to Entanglement is analogous to conservation of an observableconservation of an observable
If 1 photon “decays” into 2 photons, If 1 photon “decays” into 2 photons, energy & momentum of the system must energy & momentum of the system must be conservedbe conserved
If we know the energy of the initial photon, If we know the energy of the initial photon, and one of the others, we know the energy and one of the others, we know the energy of the final photon with absolute certaintyof the final photon with absolute certainty
Entangled!Entangled!
How is it experimentally prepared?How is it experimentally prepared?
Perturbation to the ground state Perturbation to the ground state Hamiltonian by the 3-photon non-linear Hamiltonian by the 3-photon non-linear term is proportional to term is proportional to ΧΧ(2)(2) and for the 4- and for the 4-photon term photon term ΧΧ(3)(3)
Media with high Media with high ΧΧ(2)(2) or or ΧΧ(3)(3) can produce can produce entangled photons entangled photons
How is it experimentally prepared?How is it experimentally prepared?
Laser Laser
Signal Idler
High ΧΧ(3)(3) media
Signal
Idler
Laser
High ΧΧ(2) media(2) media
Typical mediais Barium Borateor Lithium Niobate
Typical media is Lithium Niobate, doped fibres, and Rb vapour
Properties of entangled beamsProperties of entangled beams
Every pair of entangled photons are created at Every pair of entangled photons are created at different times & positions in the media, different times & positions in the media, therefore each individual beam is non-coherenttherefore each individual beam is non-coherent
Because both photons in a pair are created at Because both photons in a pair are created at the same time and transverse momentum the same time and transverse momentum entanglement/conservation - exhibits high inter-entanglement/conservation - exhibits high inter-beam coherencebeam coherence
Signal
Idler
Properties of entangled beamsProperties of entangled beams
As incoming laser becomes spatially As incoming laser becomes spatially smaller, spatial entanglement is lostsmaller, spatial entanglement is lost The two photons are entangled with the The two photons are entangled with the
incoming photonincoming photon Small laser size – infinite spatial frequency Small laser size – infinite spatial frequency
spectrumspectrum Can’t predict third photon’s spatial frequencyCan’t predict third photon’s spatial frequency Unentangled!Unentangled!
u=ui
u=u1
u=-(u1+ui)
How can it be used for imaging?How can it be used for imaging?
Want to use the higher order coherence Want to use the higher order coherence properties of sourceproperties of source
We want to use both beams for the We want to use both beams for the measurementmeasurement
We want to measure amplitude & phase of We want to measure amplitude & phase of objectobject
Detector
Detector
Object
How can it be used for imaging?How can it be used for imaging? Ghost-imagingGhost-imaging
Signal Beam
Detector
Non-linear Media
Idler Beam
Laser
Object
Detector
Intensity = Coincidence counts between detectors = Transmission function of object
Spengler
Surprise!Surprise! We are only using spatial “entanglement” We are only using spatial “entanglement”
Signal
Idler
We can create a classical, spatially “entangled” source
Differences between the twoDifferences between the two
Quantum entanglement exists in both Quantum entanglement exists in both momentum and position – near field and momentum and position – near field and far field. Correlations exist only in near far field. Correlations exist only in near field or far field.field or far field.
Visibility of object information is increased Visibility of object information is increased in Quantum schemein Quantum scheme
New directions?New directions?
Phase imagingPhase imaging Hanbury-Brown/Twiss Hanbury-Brown/Twiss
scheme cannot scheme cannot measure phase of measure phase of objectobject
Can we reconstruct Can we reconstruct phase using ghost phase using ghost imaging?imaging?
Detector
Detector
New directions?New directions?
Degree of spatial entanglementDegree of spatial entanglement Can we use the higher order coherence Can we use the higher order coherence
for funky things?for funky things?
ConclusionConclusion
Ghost imaging is a system that uses Ghost imaging is a system that uses higher order coherence to image objectshigher order coherence to image objects
It is not restricted exclusively to entangled It is not restricted exclusively to entangled light sources, but entanglement increases light sources, but entanglement increases quality of imagequality of image
Sources of entanglementSources of entanglement
Four wave mixingFour wave mixing 2 beams into media with high 32 beams into media with high 3rdrd order non linearity order non linearity
ΧΧ(3)(3) produces 2 entangled beams out produces 2 entangled beams out Performed in a Rb vapour cellPerformed in a Rb vapour cell
Spontaneous parametric down conversionSpontaneous parametric down conversion 1 beam into media with high 21 beam into media with high 2ndnd order non linearity order non linearity
ΧΧ(2)(2) produces 2 entangled beams out produces 2 entangled beams out• Performed in a birefringent crystalPerformed in a birefringent crystal• Two beams commonly called SIGNAL and IDLERTwo beams commonly called SIGNAL and IDLER• 1 in 101 in 1066 photons undergo this process photons undergo this process• Conservation of energy and momentumConservation of energy and momentum
Spontaneous Parametric Down Spontaneous Parametric Down ConversionConversion
Generates photons that have no spatial or Generates photons that have no spatial or temporal coherence in each individual temporal coherence in each individual beambeam We can’t use an individual beam to obtain We can’t use an individual beam to obtain
object information – non coherentobject information – non coherent But it does have high 4But it does have high 4thth order coherence order coherence Intensity CORRELATIONS!Intensity CORRELATIONS!
Imaging objects with detectors that Imaging objects with detectors that have “no” spatial resolutionhave “no” spatial resolution
“Bucket” detector – no spatial resolution
Light
Outputs photon number, but not position
We can image this object using ghost-imagingMarginal Intensity:
Object
121)2(
2 ),()( dxxxGxI
SimulationsSimulations0.1 mm Pump size
Co
inci
den
ce C
ou
nt
Rat
e
Idler Detector Position
EntanglementEntanglement
So as entanglement increases (because So as entanglement increases (because pump size is increasing), fringe visibility in pump size is increasing), fringe visibility in interference experiments also increasesinterference experiments also increases
This is one way in the literature that they This is one way in the literature that they define “Degree of entanglement”define “Degree of entanglement”
Phase ImagingPhase Imaging
Imaging of phase objects has been attempted – no Imaging of phase objects has been attempted – no retrieval attemptedretrieval attempted
Can we retrieve the phase?Can we retrieve the phase? Classical optics IntensityClassical optics Intensity
Ghost-imaging IntensityGhost-imaging Intensity
If we assume that , then the two equations If we assume that , then the two equations become “equal”.become “equal”.
dxesiu
xtsiu
xtuIxsi
s
ui
sisi
sis
)(2
1111*
~ 112))(
2())(
2()(
211 )( ssi ssi T.I.E
ResultsResults
Ret
riev
ed
Ph
ase