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More specifically, my interest is in the development and application of strongly correlated light, which are the building blocks of technological applications such as quantum spectroscopy, novel sources of quantum light (lying beyond the classical description).  
More specifically, my interest is in the development and application of strongly correlated light, which are the building blocks of technological applications such as quantum spectroscopy, novel sources of quantum light (lying beyond the classical description).  


== Emitter of quantum light ==
== Emitters of quantum light ==


The concept of ''quantum light'' rises from the counterposition to the ''classical light''. While the latter is well described by the classical theory of electromagnetism, i.e.,  the theory formalized by Maxwell, the former is not. In fact, quantum light has properties that are not predicted and cannot be described with the classical theory. Perhaps the most important of them is the capability of quantum light to display the so-called ''antibunching'', which is related to the way in which photons in a beam are separated in time. A laser (which is a classical source of light) emits its photons in a random way, which means that once a photon is emitted, we have no idea when the next one might come: it could follow immediately, or it can be emitted a very long time afterward. Such a random behaviour is well described through a Poisson distribution of the emission times. On the other hand, sources of quantum light are able to emit their photons in a more organized way, namely, the emission of a photon gives us some information about the time at which the next photon will be emitted. Thus, when the photons emitted by a quantum source are more separated from each other than they would if they had been emitted by a laser, we say that these photons are antibunched.


Using quantum emitters to excite optical targets opens an infinitude of possibilities and new behaviors, as the excitation itself brings to the target a quantumness, which otherwise had to rise from the internal dynamics of the driven object. Furthermore, the correlations between the photons (the way in which the photons are organized in time) can be exploited to unveil the internal structure of the driven system, thus allowing the development of quantum spectroscopic techniques.


== Polaritons ==
== Polaritons ==


Exciton-polaritons (or simply polaritons) are pseudo-particles arising from the strong coupling between a photon and an exciton (an electron-hole pair), which live confined in two dimensions inside a semiconductor microcavity. Polaritons inherit properties from their constituent particles, such as the lightweight from its photonic component and the interacting character from the excitonic counterpart. As such, polaritons can be thought of as interacting photons on which quantum information can be encoded, and which can be transported along great distances. Besides, their high-efficiency operation takes place in the micrometer scale, which place them as an interesting platform to develop quantum technologies.


== Coronavirus ==
<!--
==Outreach==


 
* Quanta Magazine: You can pitch ideas by filling this [https://www.quantamagazine.org/contact-us/ form].
Using the data that the UK goverment is making [https://www.arcgis.com/apps/opsdashboard/index.html#/f94c3c90da5b4e9f9a0b19484dd4bb14 available], updating it on a daily basis, one can fit the number of cases (of both infected people in different regions and of deaths across the island) $n(t)$ as a simple equation
* Scientific American: The submission guidelines are [https://www.scientificamerican.com/page/submission-instructions/ here].
\begin{equation*}
* Wired: You can pitch ideas by sending an email to submit@wired.com.
n(t) = n_0 \,\chi^t\,,
-->
\end{equation*}
where $t$ is the time in units of days and&nbsp;$n_0$ is the number of cases at ''day 1'', which is defined as the day where the first deaths were reported (we started with six deaths), and&nbsp;$\chi$ is the rate at which the cases increase from day to day, namely&nbsp;$n(t+1) = \chi n(t)$.
 
At the early stages of the outbreak, while the government was still trying to tackle the pandemia with the so-called [https://en.wikipedia.org/wiki/Herd_immunity ''herd immunity''], which in practical terms it means that no action was taken, and the contagions was left free to propagate. This measure was in the opposite direction that Europe was taking, where the mobility restrictions were starting to appear. At this early stage, the evolution of the cases was as shown in the figure below, which is shown in logarithmic scale:
<wz tip="Early stage of the pandemia in the UK">[[File:Covid-UK-early.png|600px|center|Early stage of the pandemia in the UK.|link=]]</wz>
The open circles represent the data and the dashed lines correspond to the Eq.&nbsp;(1) with the following parameters:
 
{| class="wikitable" style="margin: auto; text-align: center;"
|
|$n_0$
|$\chi$
|-
|'''Wolverhampton'''
|2.55
|1.31
|-
|'''Birmingham'''
|1.36
|1.44
|-
|'''London'''
|86.96
|1.34
|-
|'''England'''
|315.25
|1.27
|-
|'''Deaths in the UK'''
|7.14
|1.39
|}
which means that

Latest revision as of 12:11, 11 July 2020


Research Fields

I study the interaction of light with matter.

More specifically, my interest is in the development and application of strongly correlated light, which are the building blocks of technological applications such as quantum spectroscopy, novel sources of quantum light (lying beyond the classical description).

Emitters of quantum light

The concept of quantum light rises from the counterposition to the classical light. While the latter is well described by the classical theory of electromagnetism, i.e.,  the theory formalized by Maxwell, the former is not. In fact, quantum light has properties that are not predicted and cannot be described with the classical theory. Perhaps the most important of them is the capability of quantum light to display the so-called antibunching, which is related to the way in which photons in a beam are separated in time. A laser (which is a classical source of light) emits its photons in a random way, which means that once a photon is emitted, we have no idea when the next one might come: it could follow immediately, or it can be emitted a very long time afterward. Such a random behaviour is well described through a Poisson distribution of the emission times. On the other hand, sources of quantum light are able to emit their photons in a more organized way, namely, the emission of a photon gives us some information about the time at which the next photon will be emitted. Thus, when the photons emitted by a quantum source are more separated from each other than they would if they had been emitted by a laser, we say that these photons are antibunched.

Using quantum emitters to excite optical targets opens an infinitude of possibilities and new behaviors, as the excitation itself brings to the target a quantumness, which otherwise had to rise from the internal dynamics of the driven object. Furthermore, the correlations between the photons (the way in which the photons are organized in time) can be exploited to unveil the internal structure of the driven system, thus allowing the development of quantum spectroscopic techniques.

Polaritons

Exciton-polaritons (or simply polaritons) are pseudo-particles arising from the strong coupling between a photon and an exciton (an electron-hole pair), which live confined in two dimensions inside a semiconductor microcavity. Polaritons inherit properties from their constituent particles, such as the lightweight from its photonic component and the interacting character from the excitonic counterpart. As such, polaritons can be thought of as interacting photons on which quantum information can be encoded, and which can be transported along great distances. Besides, their high-efficiency operation takes place in the micrometer scale, which place them as an interesting platform to develop quantum technologies.