in nineteen fifty six hand bring brands standard the scientific community when he reported the

photons emitted by serious the brightest or in the night sky had a tendency to

write together in client on these detectors

that is to say unlike cars on the highway or people passing by or any

other randomly distributed classical objects whose time of arrival would be recorded like this

and bring brian and is mathematician calling twist find out the photons from a thermal

source are detected like this actually more like london buses

there is a way to have photons arrive like cars or people one can use

a laser instead of a chaotic source

the first type information comes from single photon images like a quantum dot the produce

false ones which avoid each other

the lower proposed a consequence g two defined as shown here to describe these situations

g two is equal to one for uncorrelated events

it is greater than one for circle bunching events where photons are clustered it is

more than one ideally zero for so called anti bunching events when photons avoid each

other

for instance one can compute g two from the lighting dated by a quantum dots

in the micro cavity just the following spectral lines right one would find a value

close to zero as the emission is anti bunch this is when detecting we'll phones

on from the system

but what if we select only those in this frequency window is that each to

the same as when detecting at all frequencies one can also correlate photons from two

frequency windows experimentally this is an easy thing to accomplish one million supposes the filter

before catching forms ones

theoretically however such questions are extremely difficult to resolve despite the best efforts of yours

since the links nineteen seventies only the force of heavy algebra and various approximations will

be you results and then only for particular cases of simple systems

in physical review letters we have recently presented a way around this obstacle and show

how to readily computed g n of frequency filtered photons with no restriction whatsoever on

the number of phones or on the type of system

in the new journal of physics we apply this formalism to a wide class of

fundamental quantum images for the case of two phones what coincidences

in this short movie we will show some of the results for the case already

discussed of a two level image or in the cavity

this is the spectral shape again and we're going to present correlations of photons at

all frequencies

this is the results we call this a two photons spectrum

in blue of the anti bunching correlations in white photons are uncorrelated in read their

batch

that is nigh bring our system into strong coupling by making the cavity of better

quality this results in a so-called robbie tablet we see that in the two photons

spectrum new patterns of here when the photon lifetime is very long an incredibly rich

landscape of correlations emerges

to give a qualitative idea of the most important features that just bring in the

level structure of the system the so-called jane's cummings latter horizontal and vertical patterns are

accounted for by successive emissions between this study

this cascade is bunched this sequence on the other hand or this one or anti

but as the system has to change its internal state to shift levels in this

way

more perplexing are these features and also these

let us consider the anti diagonals that correspond to direct two photon emission this relaxes

energy conservation since only the sum of the energies is fixed as the intermediate level

is skipped over we call this type of two photon emission a leap from prior

to photon emission is difficult to observe in general

we shall have to reveal it and make it obvious

there are countless configurations to revisit with this novel technique for instance this shows how

the correlations remap when the quantum dot is teaching from the cavity

and this shows what happens when increasing the pumping right

we illustrate our last example with an important remark while a perfect detector resolution can

be assumed for single photon spectra the filters line width is an integral part of

frequency result photon counting to narrow filters give true results

well blue ones are the features as shown here

and of course in the limit a very broad filters the conventional results of hand

brown and twist is recovered the study of we'll the other frequency ranges is josh

at its beginning