material science at Potsdam in Germany and from there well slack is one of the
mecca's now of fast time photochemistry so he's come to take a postdoc at our
place and to use the accelerator synchrotron x-ray sources to see what he
can do with the problems that he's interested in so today he'll talk to you about catching light a very novel
approach to problems of solar energy so Kristian thank you very much
so thank you very much for the kind introduction and also thank you all the
organizers for really inviting me here I have to say this is my first time to
give such a public lecture and it's really it's a really a great honor to do
that here and I really I I had my PhD
defense about a little bit less than two years ago and I have a little bit of feeling like at the the PhD defense
right now so I haven't been so nervous for a long time but yeah so here's the
topic of my of my lecture catching light
so no this isn't haha sorry so catching
light making the most of solar energy so when I guess you have seen this poster
or this advertisement which the slack graphic designers dip here so which this
baseball guy catching the ball of light so I have to tell you this is not
actually what we do here so this is not actually how we catch the catch the light so I would like to tell you about
how we are planning to use San Francisco Giants to get more solar energy but this
is not what I'm going to tell you about so my talk is actually going to be about dyes so so here's a here is just a
picture which I which I got from the internet so it's a it's from from the Indian market so different dyes I guess
you all know a little bit what the dye is it's something which gives a color
it's a compound or chemical compound which gives a lot of color and maybe you also know that a color of a material or
a chemical compound depends on the how this material interacts with the light like how it
absorbs what what kind of light it's absorbs and what kind of light it reflects so I will tell you about how we use this
dice to catch light and when I talk about catching light and I mean about how this ties absorb light and what
happens next so here is a short outline
of my talk so I will give a short like a motivation why we should care about
solar energy and why do we need actually catch more light I will tell you about
how the dye is doing it and how we can use dyes to actually harvest these
photons and then thirdly I will tell you about okay what we are doing here it's
like and how we can actually use the facilities here and maybe know that
there are this the x-ray science to actually study these processes taking place in dyes so to start with here is a
figure which I guess social something you all know so this is a world total
energy production over a few tens of years and as you see it's constantly
growing so that so the unit's here are
the mega tons of oil equivalent so this kind of at year 2012 the world consumed
energy which was about 13,000 million of
tons of oil equivalent so and as you know also most of it comes from a fossil
fuels and this trend is expected to
continue so it's expected that the energy production it has to grow and it
has to double by the year 2050 so and this is not sustainable because we all
know that we don't have enough fossil fuels to actually do that they will run out at some point so but there is a good
news we have a lot of solar energy so every year
about 70 million mega tons of oil
equivalent energy is reaching the Earth's surface by this by some with
sunlight so this is about 5,000 times more energy than we are using annually
right now so there it's a lot of energy and of course the question comes ok can
we harness this energy and if you can do that then we have a we have a very
powerful energy source and it's nearly infinite because the Sun will hopefully stay here for at least few billion years
so the question is can we harness the solar energy like can we just turn this
Sun sunlight into electricity and for this the question is actually yes we can
I guess you all know about solar cells so this is here the typical silicon
based solar cells and this is these are getting more and more popular and you
see that in recent years there is a figure of the of the production of
electricity by the solar cells which has been exponentially growing over few years and as it is growing that the
price of the solar cells are also increasing exponentially so this is happening right now so more and more we
are producing actually electricity from solar from solar from sunlight directly
and by the year 2050 again it's expected that this will be one of the main
sources of electricity so this is really
a great news and these are really great devices however I will show you another graph so this looks very similar like
the one I showed you a few slides before and this is final energy consumption
over a few tens of years and you see that about 18 percent of this is used as
electricity and most of it is still used as fuels so it's it's very likely that
this ratio will change in the near future in the
favor of electricity because more and more like electric cars and the electric motors will become more and more spread
but it is very unlikely that we can substitute all our energy consumption
what we get from fuels with electricity so it seems that we also need fuels and
the question is okay can we get views from Sun can we get create solar fields so-called
and this is now a really a kind of a
dream what many people have had for a fall for several years to have this kind
of so-called hydrogen society so to use sunlight and water and to create from
this hydrogen and oxygen and so that you can have a clean source of hydrogen and
you could so hydrogen it's a it's a
really good fuel so it's about three times more energetic when it's when it's
a pressurized that's around the bars so it contains more energy per weight then
then Casa lean and it's about 200 times more energy dense then leave to my own
battery right so this is a huge advantage so so batteries are great we
need more and more batteries but you see that actually their energy tends it is rather low compared to the fuels
secondly hydrogen can naturally stored so this is this is not the case I mean
we can put it electricity to the batteries but one needs a lot of lot of batteries to do that and of course it
will be a clean and carbon fee so the really the the question is so can we
have a such a device so which takes sunlight and water and
turn it into a hydrogen and oxygen so this is now a problem many
researchers and many scientists are working right now actually around the world and they have come up with with
new type of solar energy devices so which I have called a photo
electrochemical devices so this kind of devices you can use them as solar cells
so you can use them to create from sunlight electricity and they are they
are great devices they are actually now starting to maybe compete with silicon
based solar cells they have some advantages like there have a very low
production cost and investment costs and what is very important with this kind of
chemical electrochemical devices is that actually you could design them so that
they split water under sunlight so with
these devices you can design cells which split water into hydrogen and oxygen so
directly from sunlight and water so this is now very much in the research stage
so these are the sources you could in principle by but this is under a very
heavy research right now so these devices here these electrochemical devices they have a one thing in common
that they all used dyes so in all of this there is a dye is an important
component which is catching the light so and I will tell you now about how these
devices work and what the dyes are actually doing in there
so to do that I actually start with the with a normal silicon based solar cell I
don't know how much you know about this but it's it's a simple device so it's in
principle it's made out of a silicon so it's the same material like transistors are made out of computers so
in a silicon-based solar cell if a light hits silicon material what
happens history is he created the electron and a hole so charges are created in the
silicon material so in a normal state silicon has just containing a lot of a
lot of electrons they're bound to the do the atoms and they cannot conduct charge
but after the light absorption electron is promoted it gets more energy and it's
free to move in the in the material and at the same time where the electron was removed there is a vacancy of electron
which can also move around at these are the charges which can move around in the silicon so now the silicon is engineered
in such a way that these charges they separate in a material and electron
reaches one electrode and the whole so-called hole reaches to another electron and this means that in
principle you have a device which creates electricity so now you could like connect some kind of external
device to your electrodes and you could use it you could use the solar cell to -
yeah for the electricity right so that's
what in principle happens in the silicon based solar cell so now in in this
electrochemical devices so here I have a schematic picture of this one electrochemical device in principle same
processes take place but instead of having a silicon material there are
three different type of components in there so naturally there is a there is a
dye in there and die what it does it absorbs light right and
like in silicon in dye a hole and the electron is created but now different
from the silicon based solar cells these charges they cannot move around in a dye so in order to discharge
us to separate they have to move so the electron has to hope to this kind of a
nano porous titanium oxide which is a which is a semiconductor which can accept this electron and then from this
titanium oxide the electron can move to a electrode a hole on the other hand
this can be captured by the electrolyte which is a kind of a solution containing a chemical compound which can accept
this kind of this a hole and can lead it to the electrode so in principle the
same processes take place here and in the silicon solar cell only here that
the creation of the charges and their separation are kind of divided into a
different between different materials so and this makes this device a very
versatile because you can engineer this you could chemically engineer these different different dyes and different
semiconductors and electrolyte to make this work as you like now looking more
closely how this device actually looked like so here is this here is this this
nano material titanium oxide which contains dye so there are dye molecules
on the surface of this kind of titanium oxide nanoparticles so this is a very
small particle it's like usually now around 10 to 20 nanometers diameter and
it contains actually hundreds of time'll occurs on this surface if you look more
closely than i could see so this is a dye so this is a typical dye molecule how it looks like so to tell you more
about these dyes I show you that so here
is the absorption spectrum visible light absorption spectrum of a dye so this is
a red dye you see this is the visible spectrum and you can see that it
absorbs here it's absorbs only a little bit in the red range but it's absorbs more in the
green and blue range and therefore the dye it's a red colored this dye it's the
chemical formulas here so it's a it's a complicated looking structure but it's
actually not important what it exactly is important is that in the center here
you see there is a routining that's a metal that's a metal atom in the center
there ruthenium it's a noble metal and around this metal there are different
chemical groups which record which we call ligands so it's a dye which
consists of a metal central heavy metal and around this it's like carbon nitrogen different
light light atoms so in principle you can have a lot of different dyes I mean dyes can have a very different chemical
compositions but it has been shown that this kind of dies actually they work
very efficiently in these devices so that's why I'm showing it now how does
this dye actually work at the molecular level here if this dye absorbs a light
then electron from this central metal Rutina matin is transferred to a ligand
so there is a charge separation happening already within this molecule
so there is a vacancy in the metal and the electron is moved at the ligand now
in this kind of excited state if your dye is now attached to this nanoparticle
this electron at the ligand which is at the edges of this molecule it can hope
it can hope to the titanium oxide nano particle and here now it's when it's on
this particle it can travel along and hope from one nano particle to another and reach the
so that's how it happens so and it's similarly this hole here this hole can
hope to the to this electrolyte to the solution which is in there so the solution can cap it can capture
the hole and what you see is that you end up with a die in its initial State
before it actually absorbed the photon so so you end up again with die in a
radial state which means that it can absorb again a photon but you have in
your system you have two charges traveling so you have a which can create for example if you if you do this dies
in a in a solar in a in a solar cell device it can create charges so this
charge let's have a link they can travel to the electrodes and through your external device for example recombine
again creating a energy so in principle that's how at the
molecular level this tie works so it's kind of like a source of charges so it gives electrons and and holes and which
can then create electricity so yes but
what determines actually the efficiency of this this tie so I right now I just
told you that okay these processes are happening but is there something else what can happen
so if the dye works as it should then this electron hopes to the titanium
oxide so that's that's that's this is the process which is what we want
this will create electricity for us this will make the device efficient however
this process it's competing with the
other process which is a back transfer of this electron to the back to the
metal so if this happens if your electron goes
back to the metal then there is no electricity created so your your this
all just the photon which you came into your your die it just creates heat so no electricity so this in that means
inefficient so your device doesn't work in principle your your devices in a short circuit so what it means that
these two processes actually are always competing in your device and the the one
which is faster that one wins so although this process they're both
they're all possible there and they both can energetically take place there the
dynamics matters so what matters also is which one is faster so in typically in
case of this tie this process is about
100 femtoseconds to 10 picoseconds and
this packet transfer is about 100 nanoseconds so this means that this
process is much more faster and takes place so to give you the idea of the
time scales and what these numbers means so one second is about the time a light
travels from Earth to Sun sorry to moon from from Earth to moon nanosecond
which is 10 to minus 9 seconds is about the time light travels one foot like 30
centimeters so this is a much shorter time scale so the further so one
picosecond which is 10 to minus 12 seconds that
about the time a light travels about the three with hairs three widths of hair so
this is 300 microns and if you go to town to femtoseconds this is about a
light travels are like a length of a virus so it's it's smaller than a cell
so this is you see the very fast processes here now so I'm coming to the
part so this was in penal in a short
summary how this devices work and what kind of elementary processes take place
in there so what we did now we were thinking okay ruthenium nice ruthenium
dyes are very nice they are very efficient working nice but they are rather expensive actually so because of
this ruthenium metal you know it's it's a noble metal it's a very rare metal and
if you want to for example produce these devices maybe on a global scale
it will be you don't maybe probably have enough ruthenium on earth to do that so
that's of course a problem so what you were thinking okay but what about iron
so iron is a very abundant metal it's one of one of the most abundant metals
on earth if not the most abundant and it's so therefore it's very cheap and if
you look at the periodic table you see that iron is just above the ruthenium so that means that it's the the the
chemical properties and the properties of of these two dyes they are rather similar actually as you see these
molecules they're exactly the same except the metal so they can create same
chemical bonds that can create the same chemical structures this is one is also
it's a very strong light absorber so which is very important for efficient dye and it's of course it's cheap so we
were thinking okay maybe we can use iron instead why not and this we and when now when we tried
that okay in ruthenium this process takes 100 nanoseconds but in iron it's 100
femtoseconds so it's 1 million times faster so why is that it's it's it's the
same chemical structure but 1 million times faster this back transfer of
electron and this dye just doesn't work it just doesn't work it only creates
heat doesn't provide any electrons if you use it so our question okay what is
the mechanism actually what determines this timescale can we understand this
and how we can understand this
experimentally what is the challenge here so the challenge is that if you
look at this molecule molecules are right are very small so this bond distance here is like 2 times 10 to
minus 10 meters so this is about what is
a free throw distance compared to the earth to the Sun so that's how small
molecules are so so this is our way away from the human scale so when this is
what we have to distinguish in we have to understand okay is the electron here or here secondly of course these are
very fast so 100 femtosecond is this process so this is again if you compare
it to 1 minute it's like roughly like 1 minute is to 1/4 billion years so like a lifetime of
Earth so this is so fast process taking in so small scale how can you actually
see it like what's what's happening there at all right and well fortunately
we are at SLAC right so it's actually no problem
actually it's easy so maybe you maybe you know this a little bit so here is
that this is the slack site and there is this one suspiciously a straight line
here which is a linear accelerator of slack and and really a brilliant
scientist here it's like so I will zoom in so they use this linear accelerator
to create ultra short and ultra intense x-ray pulses so you have a accelerator
here so you have electron punches which are accelerated almost to the speed of light and then when they are at the
speed of light they are going through this kind of a magnetic periodic structure where this electron bunches
wiggling creating x-rays and amplifying them interacting with the x-rays as they
travel through the undulator creating a very short very intense x-ray pulse and then here there are the experimental
stations which can use these x-rays for four different experiments and that's
what we are doing so here I show
actually here is actually pulse here is the pulses that that's where I sit usually and we are here okay so how else
LS how this accelerator how it can actually do this so here is a
electromagnetic spectrum and if you look where the x-rays are the electromagnetic
waves else unless the leenock coherent light source here is creating the
wavelength of these x-rays are about the scale of item or the bond length so
that's where the sensitivity comes to the to the electron density in a
molecule because the x-rays have the same wavelength as the the bones as the items the distances of
bones or the radiuses of items leaks rays are sensitive actually to the to
these electronic densities in the in the molecule and secondly these x-rays are
coming with ultrashort pulses so they are shorter than 100 femtoseconds so
this means that if you think of your pulse as a shutter of a camera or as as
a stroboscopic light it's it's it's it's so short it's so fast so it can take a snapshot of a very fast process so
that's why LCLs can see this process and
so how we actually do this experiment is that we take we take a lot of these
molecules actually they are in in a solution like that so it's a it's a very nice colorful solution we use it and
actually we we run it in a jet so it's like as we create a little stream of
liquid which we then use in an experiment so with this little stream of
liquid first we take laser pulse come this it's ultra short it has to be short
it has to be also short in the time scale of the process we want to study and we come this laser pulse and we
excite all these molecules maybe not all of them but a lot of them so now after
that we come with the extra pass so we come and hit this stream of liquid
liquid jet we come with and hit with a filter extra pass which is also very short duration and it comes a little bit
after the after the laser pulse so it's actually well defined time delay between
the laser pulse and the x-ray probe and this this time delay here of course
gives us the time that's how we clock the time of how the process wolves so now we repeat this many times
actually we do this pump probe pump probe until we have a clear image of what takes place and then we shift the
time delay we do the pump pump probe again and that's how we create the movie so we like it change the time delay
between the pump which in each which initiates the process and then with the
x-rays become and provoke probe the system after a defined time delay that's
how we know for example within which state our system is after let's say 100
femtoseconds we excited it so then we know what what's taking place in there that's how we great we do this a very
many times we change this time delay between pump and probe and then that's
how we get the movie that's how we get the movie of how this electron is actually moving around in this molecular
yes and okay here I you don't have two pictures actually from the LCLs so this
is kind of how the experimental hutch looks like when we're doing experiments so you see it's a huge mess this is so
that's where the light is this is actually the experimental chamber and that's where we have we have a jet
running so why the light disturbed us this is just a lamp actually right now here there is no x-rays or or laser in
in there and x-rays they're coming kind of out from the out from this from this
wall and that's where we do the experiment and this when we have x-rays
and laser on here actually we we sit in a control room in a comfortable control
room and look at the screens and hopefully collecting a nice data and we
are collecting nice data then we are all happy and eating cookies and drinking
soda but if not then we are all running around and and shouting each other but
yeah usually it's we get something okay
so what do we actually learn from from this so from this experiment so we
learned that in an iron die so when we do this excitation and we separate these
charges we take the electron from the iron and put it at the ligand so what
actually happens is that it's not going to the to the its initial state very
fast there is an intermediate state in there between so the electron it's
moving back to the metal but it's not at the same it's not it's not filling the
hole at the metal it's it's going to the metal but it's still at its it has a different shape it has a different
energy and this state it kind of acts
like a like a ladder you know that's how the how it can step down so so this this
is the process which is very fast so this this is the the process which which
takes the electron from the ligand and put it back to the metal although it
doesn't put it at the same place that the metal doesn't fill the hole in there it still goes back to the metal and
makes this molecule inactive so cannot it cannot you don't have the electron at
the ligand and it cannot move to the titanium oxide so and that's just this
is not that's not what happening in ruthenium in ruthenium actually this
state is much higher we find out and so there is just just it's not
energetically it's not possible that it's it jumps there so that's the reason there is this kind of intermediate state
okay so of course we were thinking further
everything okay can we do actually something about this now if you look at
these two states they have a they have a rather different electron distribution right so so here as the electron at the
ligand that here it's at the metal so and now you can imagine because these electrons they are at different places
in the molecule they have a different shape of course they interact differently to the ligands in there
around there so they feel different forces from the ligands and if you actually maybe if you manipulate what
kind of ligands you have there in your molecule you can change the forces is
different to these electrons field and what is the relative energy so our
question is can we actually control this excited state dynamics and can we
somehow engineer this excited state chemistry so what's happening in there
and that's what we did so this is the
initial molecular set what we had which has a very fast decay to this metal
center state now when we substitute this this one ligand here with the to this
kind of carbon nitrogen carbon nitrogen ligands we see that we push up this
state this this metal center state in energy and if we substitute this second
ligand here with a carbon hydrogen carbonate in a group we even push it up
even further so this means how here okay
it's still very fast it still doesn't work but actually here so these states they are very close together so you can
still have a transition from from this
to here but because the states they're closed and there is like a barrier
between this going from one to another this process is actually much faster so
it's actually 100 times faster here so this is quite good so this all almost
works not quite it's it's still the life time here it's still way shorter than in
a ruthenium compound but this just shows you how actually one can engineer these
dynamics in this molecules and ties to maybe make them more efficient right and
actually here I come already to the summary of my talk so so there is a
major scientific challenge here we are facing right if you want to make these
devices work and efficient we need to know how to engineer this charge
separation dynamics in this flies in these photosensitizers and if you know
that we can use them to more efficiently catch the light right and even further I
mean I didn't tell you about I didn't tell you about how this device is exactly work but to make these devices
work you have to also engineer for example how how well you can like let's
say transfer a hole to the chemical compound which is doing the water
splitting for example so you need to have you need to do a lot of engineering to get this process match so that the
device works efficiently so this is a really a huge problem with lots of
chemists and material scientists are working it to understand how to do this and and the kind of molecular scale
knowledge is actually I think it really are necessary to understand how to do
this better so and secondly of course there is this huge experimental
challenge we are facing right how do you actually look at these processes now that we if you want to study them how
these electrons actually move in these molecules and how structures rearranged in in a
femtosecond time scales right so and for that we need this kind of a huge I mean
huge devices huge accelerators to do that there is no other ways to do that
actually and another thing I want to do
like a take-home message is so what makes a good what isn't necessary for a good
photosensitizer for a good diet to work in the systems so first of course it has
to absorb light very well but this is not enough in addition it has two discs
I it has to be such that this excitation leads to the charge separation so it's
not enough if you just like get hit by the ball you have to catch it right so
if you get hit by the ball okay you take the energy but it's just nothing useful
happens right so it's not enough if the dye absorbs light and creates heat it
has to absorb it and it had to be able to do with something with this two greatest choices and here's the last
slide of my my talk so I'm working in a solution faced chemistry group at pulse
so and I have a we have two bosses it's Kelly and Amy and and this work which I
actually showed it it's a lot it's a work of mostly Kelly and Robert and
Casper has have been working on this for for our many years so I I came to this
group only less than two years ago and here is a group picture we actually did
today so this is made specially for this talk so you can you can recognize these
people by these dirty clothes probably they're sitting somewhere here in this auditorium and and I also of course want to thank
all the collaborators because all these experiments they have been a big project collab collaborative efforts to make
this really work so thank you very much for your attention
okay so I think we have some time for questions I warned you that don't ask
the question until you have the microphone in your hand because this will be videotaped and we'd like to have
your question on the recording so why don't we start over here oh by the way
could you put this way the previous slide back sure so you'll notice that
the people in this picture are also the people running the microphones so you can thank them okay please sir
no thank you for the nice time I was wondering if you happen to have a copy of the video movie that you created
using the x-ray yeah unfortunately I don't have yeah I guess maybe we should
do that we haven't we haven't done really a movie so that would be of course a great thing to have yeah it
takes a certain amount of effort to reduce the data to a movie we've done that for some reactions but not for this
one yeah we have graphs I mean I didn't
show any data here that's right yeah I didn't so I maybe I should have done it but hi I have a question I'm confused
about the whole and electron transfer an electron is excited out of the ruthenium
goes to the titanium dioxide the whole goes the other way and you say the dye
molecules return to its normal state it sounds like a dye molecule is returned
to a state of charge zero yeah but we're still missing a Truong am i are they depleted am i
completely missing something well well what what do you do I mean you
kind of like yeah I mean you take an electron from a metal you put it on a ligand so the whole what I what we call
hole it's it's a vacancy of electron so then there is like electron missing so
when now from the ligand so the electron goes to the titanium oxide right there
is still a electron missing from the metal so what now happens I mean I mean
okay you can use the term hole but what you can also think of is that from this electrolyte an electron comes and fills
this so that's and that's how you are in the initial state so yeah I mean use
different languages sometimes we talk about holes and which is actually just the absence of electron but yeah so
that's how it's ends up in the initial state okay thank you and standard P V
cells you get a voltage of about 0.6 volts you know across the the junction
what do you get with in your in the in the ruthenium and in this iron and first
and second what kind of efficiencies are you far enough along to measure efficiencies I think we are talking
about here like efficiencies are around ten percent maybe so they are not as
efficient actually as as the silicon based solar so silicon resource you can make efficient but I mean the the big
advantage of this type of devices is release that they are so versatile so you can chemically engineer them to do
for example this water splitting or something and potentially in the future I mean I mean this thing depends on the
economic situation and so forth they have potential to become much more cheaper because they don't require any
this kind of you know like I mean
creating this Oh - pure silicon you know you need you need the huge factories and so on
I mean to make these devices it's actually very easy it's kind of you can kind of spray your paint them on one
substrate and and take it for it I mean what is the exact the voltage I can I
don't remember right now by heart ie
actually I haven't I haven't we haven't made it made it with iron we haven't made it into like a cellular device so
so what we did we only investigated this dye so far on page 18 what is the co t
ba okay okay I mean it's it's just the
the one chemical group of in this in this in this molecule so it's I didn't
talk about because it's just for example here yeah you're talking about for example this so I mean this this dye
it's actually it's actually a salt I think so it's a if you this TVA it's if
this is one cation I mean it's a positive ion actually which is but in a solution actually this this TVA part
it's in in the solution I believe I mean it's just CLO it's a carbon oxygen
oxygen it's like carboxyl yeah yeah
could ask another question sorry so I
was curious when you were showing the periodic table and there were some other elements besides iron that were
surrounding ruthenium have you ever gonna look at any of those other elements so far
okay here I mean when we are talking
about molecular photosensitizers so we have only looked at iron ruthenium I mean actually you
can I mean you can use different dyes or different photosensitizers for example
you can use nanoparticles photosensitizer also which we have which
we have tried to study and if you look at the other other metals here these are
metals for example which we are also we are studying the complexes of for example cobalt to look at the catalytic
or the chemical activity of these complexes but we haven't looked at like other molecular photosensitizers other
than that use manganese which is right
next door mm-hmm but generally the chemistry is the same when you go down the periodic table and it changes when you go across
so I don't know how that works with yeah I think it's about it's about right yeah I mean it's it's very I hesitate to say
something very generally right here but but it is true that this this group is kind of its kind of there it's kind of
photosensitizers and for example cobalt and manganese and they are kind of this kind of which initiate or catalyze
reactions chemical reactions
so so when you change that iron-based molecule to make the energy Delta's
better or whatever it was he did how did he decide how to change the molecule oh that's a good question I mean you're
kind of trying out a little bit I was only who's more trial and error or if there's well with with this with this
what I showed here I mean the kind of
their ID was and I think it was actually a correct ID is that so if you if you
have this let's say you have this two metal centered electron state at the metal like one is where you create a
hole and the other one is this you know when the electron goes back but it doesn't fill the hole but it's still at
the metal so these are this two different different state and having
different ligands using using this CN ligand which is actually it which has a
which has a effect to these metal orbitals that it tends to make them make
them energetically further apart so this is something we knew we know that if you
if you substitute these ligands with the C and you make these two two metal
centers electron orbitals electron States further apart and that's why we
used it and I think actually it was a correct ID
okay um so when using the I think you mentioned for the x-ray spectroscopy
techniques is it really wouldn't it be really hard to distinguish scattering atoms with little difference in atomic
number so I think that's a correct
comment but I mean what I didn't tell you here about is that we didn't look at the scattering your fix rays actually we
did a spectroscope yeah and and we used this kind of I didn't go into this
detail I really did try to avoid any this kind of technical x-ray spectroscopy with specific details but
we use the x-ray spectroscopy technique which is just sensitive to the to the
actually kind of how many electrons you have at the metal so it was we kind of
selected a technique
do your theoretical physicist friends have any kind of theory or model that
you could pursue to choose a different kind of ligand either a different number
of ligands or a different our compound yeah I mean that would be really great if you could just calculate everything
and we would know everything this is in principle yes we would like to do that
we would like to be able to calculate everything and we are actually working in close collaboration with with I mean
it's a quantum chemistry of quantum chemistry groups who are doing all this very complicated calculations but I mean
one problem with this these systems is actually that it's it's and not only
these systems but actually in general it's it's very difficult to actually get accurate description of of all these
excited state dynamics I mean this this I would I could say that with lots of
molecules for example they take this kind of ground state calculations work very well but if you if you make
expectations and you want to understand the dynamics this is very hard so this
is hard to hard to really calculate so we can calculate lots of things and we it's helpful but we cannot do the whole
we cannot do the whole calculation what
is the voltage it takes to split water into hydrogen and oxygen and how well does this match the voltage you can get
from a photo electrochemical cell I mean
when we are talking about these these water splitting devices what I was so so
it's important to to actually point out that this this is not electrolysis so this is not just like because you could
just you know put like two electrodes in a water just metal electrodes and just
if you put enough voltage you could just split your water you could do that I don't know what's the voltage exactly is
yeah yeah but yeah yeah but but with this with these systems the the aim is
actually they were due to use these to this designed you know catalytic
molecules which which can do it with like that's very low very low voltages I
believe so that so that you can drive this process with this with the source and in principle also kind of like based
on how like you look at the atoms and like can like the electrons um would
also like the distance determinations be limited because of like the presence of the K edge of one of the metals that use
sorry I didn't get this like um when so when you're using like the x-ray for
measuring like the atoms and like the amount of electrons when also like the
distance determinations like be limited due to like like a K edge of one of the metals that you're using so I mean III
sorry I didn't I didn't I just don't hear very well your question but I mean we are using like a different technique
so I don't know are you asking still about scattering or or for example or distances so yeah kind of well like yeah
yeah something yeah I mean actually I mean we don't use only spectroscopy we
have been using also like scattering which is kind of sensitive also to the chest to the like distances in your
molecule and and Vav RB we have been able to for example look directly at the structural dynamics how the how these
molecules like wobble around and what they do and also like what what actually
solvent around this is doing so there is really different things to look at so not only not only this yeah it's all
that the answers to in that case when you're using with the scattering back to like kind of like the first question how
do you like work around like it being really similar to other molecules with
little like number I mean this is a really important questions right yes I mean it is well I
can just tell you so much that I mean
it's a question of sensitivity right so we just have used this spectroscopy
technique which we which we know we have like measured like at lab before that
there is the sensitivity to this to this you know electron count at the metal and
we know that there is a there is we are sensitive to that of course when we do this experiment
so if our sensitivity is very low then we just have to pump and pump and probe
a lot of times and but yeah I mean if
you do it right if you select your system right you can you can see it okay Thank You Vicki so that's not Christian