Transcript
[0:08] okay I hello Roger it's my great
[0:11] pleasure and honor to introduce our next
[0:13] speaker sir Roger Penrose uh who will be
[0:16] talking about why the symmetries of
[0:19] microtubules in a relativity Theory may
[0:22] have unexpected implications for the
[0:24] timing of conscious actions let's give a
[0:26] round of applause to Sir Roger Penrose
[0:31] I hope you can hear me can
[0:33] you can you hear me yes oh good um can
[0:39] you see the screen we can see the slide
[0:42] and we can see you in the corner so
[0:44] everything's perfect okay yes I'm afraid
[0:48] I don't have anything nearly as
[0:49] interesting as what we just heard but
[0:52] I'll just tell you a few things which
[0:54] I've been thinking about um not
[0:58] necessarily recently either
[1:01] uh let me move on to the well first of
[1:04] all the question of symmetry and Stuart
[1:08] told me that since this session has to
[1:11] do with symmetry um and dimensionality
[1:14] and I couldn't think of anything I could
[1:16] say which did to do with that but he
[1:17] told me it was my fault that he named
[1:20] this after these Concepts so I had to
[1:23] think hard about how symmetry could be
[1:26] relevant to things that I might talk
[1:28] about and there is one thing in
[1:31] particular with regard to microtubules
[1:34] which maybe has some interest so let me
[1:36] here we has a microtubule I should say I
[1:39] should apologize for the top right hand
[1:41] corner because I gather Stuart this is
[1:43] an old slide and the idea that it had to
[1:46] do with confirmations seems to be
[1:48] outdated now but never mind about that
[1:51] this is a picture of a microt tual which
[1:53] I must have drawn a long time ago and
[1:56] you can see something about the
[2:00] uh ltis structure along the
[2:03] micral
[2:05] now
[2:06] uh I I should explain first that the
[2:11] general idea I had about Consciousness
[2:12] was a long long time ago and I was
[2:15] impressed by learning about girdle's
[2:18] theorem and that there were things that
[2:21] seemed to be non-computable that un
[2:25] understanding the quality of
[2:27] understanding seemed to be something
[2:28] that you couldn't defined in terms of
[2:32] algorithms and if that was the case then
[2:35] there has to be something since our
[2:36] brains are physical objects there has to
[2:39] be something going on in our brains
[2:42] which is part of the physics which might
[2:44] be outside
[2:46] computability and the only thing which I
[2:49] could think
[2:50] of which could possibly be a role play a
[2:54] role of this nature that be uncomp
[2:56] computability uncomputable was the
[2:58] collapse of the wave function because
[3:00] all the other features of physics seem
[3:03] to be something where you could put them
[3:06] on a computer of course make their
[3:09] parent physics depends on the Continuum
[3:11] continuous variables and so your
[3:14] calculations are always approximations
[3:16] there is a possible loophole there but I
[3:18] didn't think that was like to be the
[3:20] answer to this this puzzle that I was
[3:22] having to find something in physics that
[3:25] could be
[3:26] non-computable and I thought about
[3:27] general relativity and electromagnetism
[3:30] all these things and it didn't seem
[3:32] there was much hope because you could
[3:33] put those on the computer um what about
[3:36] quantum mechanics well you can put the
[3:38] wave function on it I I had the
[3:41] view that it was the collapse of the
[3:44] wave function which somehow had to be
[3:46] outside what you could
[3:48] compute now current understanding is
[3:51] that it's a random process um it would
[3:55] have to be something a little more
[3:56] subtle than that if it's going to be uh
[3:59] something which is involved the
[4:01] Consciousness never mind that's come to
[4:03] that question later perhaps but anyway I
[4:06] wrote this book The Emperor's New mind
[4:07] where I tried to express this idea that
[4:10] maybe the collapse of the wave function
[4:13] well in order for it to be any play any
[4:14] role you had to have Quantum me Quantum
[4:19] systems going on my brain which could um
[4:23] be sort of big enough in a sense that
[4:26] the uh uh you could preserve coherence
[4:30] to a to a significant
[4:34] level and
[4:37] I I learned about the hodin axley nerve
[4:41] transmission and I thought there wasn't
[4:42] a hope because the the signals done
[4:48] neurons would disturb the ambient um
[4:54] material in in a sort of random way and
[4:56] there's no way you could preserve
[4:58] coherence just with nerve transmission
[5:00] so I sort of Pete it off at the end of
[5:02] my book without having an
[5:05] idea but then Stuart read my book and
[5:09] told me about microtubules and the
[5:11] microtubules then were the main
[5:14] difference between the first book here
[5:16] on the left and the second one where I
[5:18] realized there might be something in um
[5:21] microt tual Behavior but I didn't have
[5:23] much idea about it okay let me come back
[5:26] to the microt tual the only thing I
[5:29] wanted to say now
[5:31] which I hadn't expressed before has
[5:33] something to do with the structure of
[5:36] microtubes and
[5:38] uh you can think of a micral lattice as
[5:42] being something like a hexagonal lattice
[5:45] which has uh three different directions
[5:48] in which it repeats itself and uh but
[5:51] then you roll it up into a
[5:53] cylinder now if you think of it locally
[5:56] then there are these three different
[5:58] directions one is
[6:00] uh when it is rolled up into a cylinder
[6:02] one is sort of cork screws around one
[6:04] way another one cork screws the the
[6:07] other way and the other one translates
[6:09] along the length of the
[6:12] microtubule now it always struck me as
[6:15] rather strange that the microt tubes you
[6:18] found here have this particular symmetry
[6:21] which goes along the the microt tuble
[6:24] itself and it's certainly it's possible
[6:27] in I gather in a dish or something you
[6:29] can construct all sorts of microtubules
[6:32] which have different numbers of columns
[6:35] you see the microtuble has 13 of them if
[6:38] you change that number to 14 or to 12
[6:42] you can certainly have microtubules but
[6:44] then they lose this translational
[6:46] symmetry they're all twisty go one one
[6:49] way or the other um but there're twisty
[6:52] symmetries why does the micr tual seem
[6:55] to have this purely seems purely
[6:58] accidental this uh translational
[7:01] symmetry along the direction of the
[7:04] microtubule and this reminded me of
[7:07] something I'd seen in some discussion of
[7:12] um
[7:14] uh um um carbon nanot tubes and you can
[7:19] have them with different all sorts of
[7:20] different
[7:21] symmetries and it seemed to be the case
[7:24] that those which had a symmetry
[7:26] translational symmetry in the direction
[7:29] of the tubes
[7:31] they would exhibit
[7:34] superconductivity and superconductivity
[7:36] at room temperature is
[7:39] something which well you can maybe they
[7:42] can do it with these nanot tubes but I I
[7:45] I not sure I can even remember which
[7:47] this article I was looking at maybe
[7:49] somebody could find it that for me but
[7:51] in the study of these carbon nanot tubes
[7:56] it seemed to be that when you had this
[7:58] linear symmetry not just the twisty
[8:01] symmetries uh the cork screw symmetries
[8:03] but at least one symmetry which is
[8:06] translational and then this was
[8:08] something present in these particular
[8:11] carbon nanot tubes which happen to have
[8:13] exhibit super
[8:15] conductivity so it's suggested to me
[8:17] that there might be some kind of role is
[8:20] played by
[8:21] microtubules
[8:23] um excuse
[8:25] me
[8:28] um and where it would make use of the
[8:31] this addition Symmetry and I can't say
[8:33] really much more about this because I
[8:34] never thought about very much more it
[8:37] just seem to me that there is should
[8:40] something which should be
[8:41] explored um maybe there is something
[8:43] particular about the
[8:45] microtubules which you find and they
[8:47] have this translational symmetry um
[8:51] which could perhaps uh accompany some um
[8:56] s some Quantum effects which could be um
[9:02] more Global than the ones we normally
[9:03] find now I don't want to say too much
[9:05] more about that um because uh really
[9:09] what I want to talk about is something
[9:11] different uh first of all let me talk
[9:13] about the uh
[9:17] Quantum uh evolution of the quantum
[9:21] State excuse
[9:24] me um there are
[9:28] uh two procedures one is this shinger
[9:32] equation you see people often when they
[9:34] talk about quantum mechanics they just
[9:35] talk about the shrodinger equation they
[9:37] sort of the collapse of the wave
[9:39] function or something which is sort of
[9:42] rather embarrassing to Quantum Mechanics
[9:44] because it's not really part of quantum
[9:47] mechanics to have a theory of that it's
[9:49] just that when it changes the quantum
[9:52] amplitudes into into
[9:55] probabilities and how you go from one to
[9:57] the other is not really explained
[10:00] in current Quantum Mechanics in
[10:02] certainly in conventional quantum
[10:04] mechanics and what just has these two
[10:06] procedures the shringer equation and the
[10:09] collapse of the wave function now the
[10:11] shringer equation tells is a uh a smooth
[10:16] um computable if you like and uh
[10:21] deterministic
[10:24] process it's like Newtonian mechanics in
[10:26] that respect but it's just the ordinary
[10:29] kind of thing you just follow the
[10:30] schroer equation and it gives you this
[10:33] um smooth
[10:36] Evolution which is
[10:38] deterministic collapse of the way
[10:40] function as we understand it is
[10:43] random uh it's a completely different
[10:46] kind of process and why do we go from
[10:49] one to the other why do we how do you
[10:51] have a theory which encompasses both of
[10:53] them at the same time there's a little
[10:55] thing which may be a point which might I
[10:58] thought about recently where people talk
[11:00] about um I think it was I'd heard about
[11:03] a lecture which had been giving given
[11:07] concerning Free Will in animals and the
[11:10] question is how could you tell whether
[11:11] the animals had free will or not I mean
[11:13] how do you know and then I began
[11:15] thinking about how what do I say about
[11:17] Free Will I mean is the collapse of the
[11:19] way function I know Stuart often says it
[11:21] gives you scope for free will but free
[11:24] will what does it really mean and people
[11:26] often talk about it well you can be in
[11:28] fact there were some of these
[11:30] experiments I believe when treat people
[11:31] tried to be as random as they could and
[11:35] the question was whether they were
[11:36] really being random or not and
[11:40] uh the free will seem to be the quality
[11:44] that you could be as random as you like
[11:46] now that really can't be the answer um
[11:49] it seemed to me that it isn't really the
[11:52] answer because if you want who ask if
[11:54] something has free
[11:55] will um well that means they're using
[11:58] their conscious experence experiences or
[12:00] conscious understanding or something to
[12:02] do what they want to do now what doing
[12:04] what they want to do depends upon
[12:07] probably some kind of process which they
[12:09] go through which um tells them that this
[12:12] is the right thing to do now I'm trying
[12:15] to say that conscious activity is
[12:17] something which goes beyond
[12:20] computability now you
[12:22] see the freedom that you have in in in
[12:27] Consciousness or the freedom of Free
[12:29] Will is not the freedom to be
[12:31] random uh that's not the point it's
[12:33] freedom to do what you think is the
[12:35] right thing to do it may be the wrong
[12:38] thing to do but what you think is the
[12:39] right thing to do and that depends on
[12:41] your conscious
[12:43] understanding so I'm trying to say that
[12:46] again it's it's not it has to be
[12:49] something which is not random it has to
[12:51] be something which is controlled by some
[12:54] kind of thing which is deeper than
[12:56] random it's non-computable some kind of
[12:59] process which is involved in the
[13:00] collapse of the wave function is the
[13:02] idea okay well let me let's move away
[13:05] from
[13:07] that sorry I'm going the wrong way of my
[13:11] pictures just a
[13:17] second okay now Quantum
[13:21] superposition let me talk about that
[13:23] first you see it's the quantum
[13:26] superposition is what you Quantum
[13:30] processes involve lots of quantum
[13:31] superpositions and they
[13:33] get uh you can have a system which
[13:35] involves an environment and then the
[13:38] environment gets too complicated and
[13:40] then you want to
[13:42] know what it's
[13:43] doing well the idea is it would still if
[13:46] you don't have the collapse of the wave
[13:48] function it would follow the process of
[13:52] quantum
[13:54] superposition now what
[13:59] F position is that if you have state a
[14:03] or a state B both of which are allowable
[14:06] States then so also is a state Alpha a
[14:09] plus beta B now Alpha and beta are
[14:13] complex numbers so they involve the
[14:15] square root of minus one and I always
[14:17] found this very remarkable because I
[14:18] learned about complex numbers when I was
[14:21] doing my uh undergraduate course
[14:23] University College in London and uh I
[14:27] didn't know anything about quantum
[14:29] mechanics at the time and I thought
[14:31] wouldn't it be wonderful if physics
[14:33] somehow used these wonderful numbers and
[14:35] the wonderful mathematics that they
[14:37] derive and it wasn't until I learned
[14:39] about quantum mechanics I realized that
[14:41] they actually do play this fundamental
[14:43] role now the thing is that if you're
[14:47] thinking of a as being some object in
[14:49] one location and B as being the location
[14:51] in another object then it's a bit hard
[14:52] to imagine how you can Alpha have a
[14:55] combination of alpha being one place and
[14:57] beta being the other place I remember
[14:59] Direct in his lectures which I went to
[15:02] uh when I was a graduate student and uh
[15:06] he tried to explain about the super
[15:08] position that he had said you have an
[15:11] atom in one place it could be in another
[15:13] place and then there were various states
[15:15] where it can be both at once and then he
[15:17] gave some explanation of why you didn't
[15:19] normally find big things like pieces of
[15:21] chalk in two places at once and I
[15:24] remember being uh distracted by
[15:26] something that was going outside the
[15:28] window and I never heard his EXP
[15:30] which is probably a good thing because
[15:32] his explanation was probably something
[15:34] to calm me down and not worry but
[15:37] um it seems that uh is something that I
[15:41] felt I needed to worry about and I
[15:43] didn't hear his explanation which is
[15:45] probably a good thing
[15:47] anyway uh let me explain that it's
[15:51] Quantum superos is very fundamental to
[15:53] quantum mechanics and it's not something
[15:56] which just says that if something can be
[15:58] over here or over there then have these
[15:59] funny looking states where it could be
[16:01] both places at once it really is a
[16:03] central part of well I thought one of
[16:06] the things that's very nice to do think
[16:08] about spin and the spin of a spin half
[16:11] particle can be described as the state
[16:15] the General State of a spin half
[16:17] particle can be described as take some
[16:19] direction in space and then it's
[16:21] right-handed about that direction now
[16:24] the thing is that there are really two
[16:26] different states or two different
[16:28] independent states of a spin half
[16:30] particle and they can be spinning
[16:32] right-handed about the upward direction
[16:34] or about the downward Direction and then
[16:36] all these different complex combinations
[16:38] of the two are represented by these
[16:42] linear combinations and they are with
[16:44] these complex numbers and you see this
[16:46] relationship between these wonderful
[16:48] complex numbers and the structure of
[16:50] space and I found this extremely
[16:52] striking and remarkable and there is
[16:55] nothing special about up or
[16:58] down and all the other combinations are
[17:00] on equal footing with them up or down so
[17:02] if you have a state like this then you
[17:04] can see that there's nothing special
[17:06] about one or the other all the different
[17:09] combinations are just as good as the
[17:11] individual ones so that's a nice example
[17:14] showing you that
[17:17] now uh much later when I started
[17:21] worrying about how to bring quantum
[17:23] mechanics and relativity general
[17:25] relativity Theory together in some sort
[17:27] of way I realized
[17:30] that you needed to have uh something
[17:33] like a collapse of the wave function you
[17:35] see the two basic principles quantum
[17:38] mechanics is this superposition
[17:40] principle which I just been talking
[17:41] about and general relativity it's the
[17:44] principle of um s principle of
[17:49] equivalence which is saying that locally
[17:52] a gravitational field can be eliminated
[17:54] by free fall and one can show that
[17:59] that these two basic
[18:02] principles are essentially incompatible
[18:05] with each other but if you try to have
[18:07] them both at once you're led to a limit
[18:10] in the time scale of the
[18:12] superposition so that this was what
[18:15] drove me to a particular
[18:18] uh lifetime for a superposition which is
[18:21] given by this formula here I learned
[18:24] later that two years earlier diosi had
[18:26] come to the same conclusion using some
[18:28] different argum
[18:30] ments anyway that gave perhaps the fact
[18:32] there was another way of doing it was
[18:34] was a additional reason for collaps
[18:37] taking it seriously but the argument is
[18:40] that if you have
[18:42] a what you have a a quantity called EG
[18:46] which I'm calling the uh well that's
[18:51] the energy
[18:55] the if you think of a superp position
[18:58] it's the
[19:00] gravitational self energy of difference
[19:02] between the two states and if it's a
[19:03] spin half particle then there there
[19:05] isn't such a think could go on forever
[19:08] because it's there's no such energy
[19:11] difference here but if you take a say
[19:14] piece of chalk and two at once then
[19:17] there is this energy difference you take
[19:19] the
[19:22] um energy the the self energy it's
[19:25] better to explain it another way which
[19:27] is at the bottom of the slide I don't
[19:28] quite know why it's it's got slid down
[19:30] the bottom the bottom of the slide um we
[19:34] have you can describe it in another way
[19:37] you could say that the two bodies you
[19:38] can think sorry you can think of a body
[19:40] in a superp position of two locations
[19:43] what is the EG well you think of that
[19:45] body um two instances of that body on
[19:49] top of each other then you try to move
[19:51] them apart to the place where they're in
[19:53] super
[19:54] position and ask how much energy would
[19:56] that cost you to move them apart when
[19:58] you consider only gravity you have to
[20:01] ignore electri electric forces your
[20:03] nuclear forces all these much much
[20:05] bigger you ignore all those other forces
[20:08] you just take the gravitational force to
[20:10] pull them apart and how much energy
[20:12] would that be and this is this quantity
[20:14] EG so that's the quantity EG okay now
[20:19] let's try and get back to the Symmetry
[20:21] Quest
[20:23] um you see if if you have
[20:27] uh a fundamental thing like this which
[20:30] is supposed to be consistent with
[20:32] relativity then it has to be consistent
[20:35] not just with general relativity it has
[20:36] to be consistent with special relative
[20:38] so if you if you're considering your
[20:40] moving frames and things the the theory
[20:44] has to work with different frames so I
[20:46] have here A Spacetime picture I'm
[20:48] imagining a body right at the bottom of
[20:50] the picture it's put into a
[20:52] superposition of two locations As you
[20:54] move up the picture they get further and
[20:56] further apart at a certain point they
[20:59] collapse to one so it goes to the
[21:01] location Q or the loation Q star let's
[21:04] say it goes to
[21:05] qar now I want to describe this picture
[21:09] in different space different frames you
[21:12] see I'm using now the symmetry of
[21:14] special relativity special relativity
[21:16] has a symmetry so I wanted to bring
[21:17] symmetry into the arguments and so that
[21:19] was the point I was doing this
[21:21] here explaining uh the fact that you
[21:24] have the symmetry of special
[21:27] relativity is little of a problem when
[21:29] you consider this this
[21:32] diosi scheme you see
[21:36] um how do we suppose this I imagine the
[21:41] body is at the bottom it's super
[21:43] superposed into two locations and then
[21:46] eventually it goes to point qar rather
[21:49] than Q in this case let's go say it goes
[21:51] to qar now if I describe this picture
[21:55] according to ordinary let's say ordinary
[21:58] description you think of your horizontal
[22:01] slices through the picture uh giving you
[22:03] what happens and it goes on chugs away
[22:05] and then at a particular moment the
[22:08] superposition becomes qar rather than q
[22:11] and then then Q has disappeared and it
[22:12] becomes q but how you suppose we
[22:15] describe this picture According to some
[22:18] Observer let's not hold an observer
[22:21] because there's nobody really looking at
[22:22] it but some frame of reference which is
[22:25] moving rapidly over to the left or to
[22:28] the the right it has to be with less
[22:30] than the speed of light but let's say
[22:33] it's the if it's moving to the left as
[22:36] you go up those are the T ones where the
[22:40] uh sorry it's the other ones these are
[22:42] the S ones where the what is regarded as
[22:45] simultaneous with regard to that frame
[22:47] of reference it would be that the slope
[22:50] up the ones you see f s s0 and S1 those
[22:55] are two uh descriptions which would
[22:57] regard as simultaneous
[22:59] to the uh Observer moving up to the left
[23:03] and that one you see the Q star would
[23:07] have become the whole state before the Q
[23:10] has actually disappeared you see there's
[23:12] still an amplitude for Q to be there
[23:15] when the whole state has become Q star
[23:17] and that doesn't make any sense because
[23:19] that means there's still a probability
[23:20] that it might be q and then it could be
[23:22] both places at once and that makes
[23:24] nonsense it's it even worse for the
[23:27] other state I suppose because that's
[23:29] moving off to the right and then the
[23:30] slope is the other way around these are
[23:32] the t's and t z and t s there's no
[23:35] problem there but when you go to T1 you
[23:38] see the one of them has already
[23:40] disappeared and the other one hasn't
[23:43] quite made it up its mind yet with it
[23:45] disappear or not that doesn't make any
[23:47] sense because it might disappear still
[23:49] and that isn't doesn't make any sense so
[23:52] the picture doesn't work the P doesn't
[23:54] work for the collapse of the wave
[23:56] function unless you go right down to the
[24:00] point0 that is to say it's the reality
[24:03] of the state was all the time the left
[24:07] hand one but what do you say about the
[24:10] superposition well to make sense of this
[24:12] you really have to have two different
[24:14] Notions of reality and I'm calling these
[24:17] two Notions classical reality and
[24:19] Quantum reality the quantum reality it's
[24:22] true that there is this superp position
[24:25] and this is the less robust kind of
[24:27] reality it's a little bit hard to pin it
[24:29] down the classical reality is the one
[24:32] which goes off to the right and that is
[24:35] uh you have to make a distinction
[24:37] between the two kinds of reality in
[24:38] order to make sense of this
[24:40] idea now um I'm not sure I got the right
[24:44] yeah Quantum reality now Quantum reality
[24:48] is really defined by a notion introduced
[24:51] by
[24:52] Einstein what I'm calling Einstein's
[24:54] dictum he says if in any well I'm
[24:58] eyesight is too bad to read it actually
[25:00] perhaps you can read it the concept is
[25:03] that if you can perform an experiment on
[25:06] a
[25:08] system and that system is not changed by
[25:11] the experiment so it leaves it alone and
[25:14] it gives you an answer with certainty
[25:17] then that gives you a reality to that
[25:19] state so this kind of reality is what
[25:23] I'm calling Quantum reality Einstein
[25:26] didn't distinguish it from any other
[25:28] kind of reality I think but it is it is
[25:31] what I mean by Quantum reality and
[25:33] that's I got 1935 I think is when he the
[25:36] state came from this is a quote from
[25:39] Einstein so uh Quantum reality is
[25:42] defined by the Einstein
[25:45] criteria and this is the kind of reality
[25:47] you have here so if you imagine a state
[25:52] of spin which might happen to be sort of
[25:54] as indicated up to the right then you
[25:58] can perform a measurement on that state
[26:00] of Spin and if your measurement is to
[26:03] say is your spin in that particular
[26:05] direction it will say yep with certainty
[26:08] yes that is my Direction but if you try
[26:11] some other direction then it's or if you
[26:14] can say you see you can't ask the state
[26:16] of spin hello state which way are you
[26:19] spinning it just looks blankly at you
[26:21] and says I don't answer questions like
[26:23] that choose the direction and then I'll
[26:26] tell you an answer now if you happen to
[26:28] choose the right direction then it will
[26:30] say yes with certainty you got it right
[26:33] if you choose some other direction it
[26:34] will just give you probabilistic answers
[26:37] depending upon how far off you are if
[26:39] you're nearly right it'll say usually
[26:41] it'll give you the right it'll say yes
[26:43] occasionally say no if you got it in
[26:45] right angle so that direction is will
[26:48] say 50% right 50% no if it's you got the
[26:51] opposite direction you will say no every
[26:53] single time so this is the where you
[26:56] have to understand Quantum reality you
[26:58] can't
[26:59] you can't ask the state what it's real
[27:01] what its reality is you can confirm what
[27:03] it is so it's a question of confirming
[27:06] rather than ascertaining classical
[27:08] reality is something you can ascertain
[27:10] Quantum reality is something which you
[27:12] could confirm if you get it right if
[27:14] you've got it wrong it will just give
[27:16] you probabilistic
[27:18] answers and it's important to make this
[27:21] distinction uh otherwise it you it
[27:24] doesn't seem to make sense of the way
[27:26] the world works so classical I have now
[27:29] a picture of the sort of thing I mean at
[27:32] the bottom it is a space Time picture
[27:34] roughly speaking so time is sort of
[27:36] going up the picture sort of sloping off
[27:39] to the right if you like going up the
[27:40] picture at the bottom we have a laser
[27:43] which is aiming a high energy Photon at
[27:47] a beam splitter or halfs mirror if you
[27:49] like and it splits the photon into going
[27:53] horizontally and going down and so that
[27:56] means that the horizontal state
[27:59] uh it hits this little lump of material
[28:02] a speck of dust or something a little
[28:03] tiny grain there it hits it and this
[28:06] thing then starts to move by the impact
[28:09] of the photon if it didn't hit it it's
[28:12] left in the same place now you follow
[28:14] the evolution of this thing as you go up
[28:16] it starts to be in a super position of
[28:18] two locations it keeps on as you go up
[28:21] into two locations and then the collapse
[28:23] happens one of them disappears and it
[28:25] becomes the other now the quantum
[28:27] reality sort of tries to follow both
[28:29] branches at once in some way the
[28:31] classical reality follows the leftand
[28:34] branch because that's what the answer
[28:36] happens to be but there is something
[28:38] kind still curiously retroactive about
[28:41] this it seems to go backwards in time to
[28:44] just establish what the reality is which
[28:47] is a kind of strange idea but it's it
[28:51] seems to be what you need in order to
[28:53] make sense of things like this this is
[28:55] sort of um Einstein f foli
[28:59] type of experiment where again it's A
[29:02] Spacetime picture the picture is going
[29:04] up from bottom to top right at the
[29:06] bottom well the left hand one is called
[29:09] Alice and the right one is called Bob
[29:11] for some reason they're always called
[29:12] Alice and Bob A and B they
[29:15] are and the they are given a spin zero
[29:21] state which that means when it's split
[29:25] into two halves Alice takes the one half
[29:29] and Bob takes the other half so because
[29:32] it could be say two electrons or
[29:33] something like that one one spins in
[29:36] some way which is opposite to the other
[29:39] one however it's not determined which
[29:42] way it spins the state the quantum state
[29:45] is that it's the superposition of Alice
[29:47] being spin one way and B the opposite
[29:49] and Alice the opposite and B the one or
[29:52] if you like that it's a completely
[29:54] symmetrical State uh and you can follow
[29:57] the evolution of it this as it goes up
[29:59] and then at a certain point Alice makes
[30:01] her measurement she chooses
[30:04] something if you can see that at the
[30:06] right top left part of the picture uh
[30:09] she measures tries to measure it uh sort
[30:12] of angled up upwards into the right a
[30:14] little bit and the state says no that's
[30:17] wrong and so Alice's State comes to the
[30:20] conclusion it must be the opposite and
[30:22] then bub State instantaneously Well it's
[30:25] worse than instantaneously because you
[30:27] have to look at the make it realistic uh
[30:30] to make it
[30:32] um consistent with special relativity
[30:36] and the only way you can do that is that
[30:38] Alice's State the quantum reality of her
[30:41] State propagates backwards along the
[30:44] past cone so you can see these sloping
[30:46] lines through this point where Alice
[30:48] makes her measurement and goes back and
[30:50] hits Bob state so Bob state becomes
[30:53] spinning the opposite way to alysis and
[30:57] that is the Quantum reality of the state
[30:59] now if Bob could ascertain what that
[31:01] state was you would be in real trouble
[31:04] because that means you could send
[31:05] signals past the light and space and
[31:08] special relativity would be out the
[31:09] window there would be no way of uh
[31:13] making sense of special relativity
[31:15] special relativity only makes sense
[31:16] because you can't send signals faster
[31:19] than light so Bob since it's Quantum
[31:22] reality Bob State Bob state but at the
[31:25] point QB I think you can see it you
[31:27] follow the diag line off to the right
[31:30] hand from the measurement Alice had made
[31:33] and it retroactively changes Bob state
[31:37] to be the opposite of Alice's
[31:40] measurement she said it measures well
[31:43] it's the same as Alice's measurement
[31:45] because it's the opposite of what she
[31:46] finds put it like that um so it's now
[31:49] become the quantum reality of Bob State
[31:53] same way that Bob makes a measurement
[31:55] even lat of analys and along his light
[31:58] cone it has influence alysis States you
[32:01] could say that the quantum reality of
[32:03] her state was already fixed by the time
[32:05] she measured it that's a pretty crazy
[32:07] picture but it seems to be completely
[32:10] consistent this tells you the quantum
[32:12] reality of the whole situation which
[32:15] completely consistent looks crazy
[32:18] because it involves these retrocausal
[32:21] effects so you have to say that these
[32:23] retrocausal effects are really there but
[32:26] they're only in Quantum reality so you
[32:28] can't really ever sort of make use of it
[32:31] in in in an
[32:33] experiment however it may be now here
[32:37] this is it goes back to the things which
[32:40] I have talked about before in fact this
[32:42] picture comes from my the emperor's new
[32:45] mind it was already there and I already
[32:47] worried about these things it's an
[32:49] experiment due to Benjamin liit where he
[32:53] um had an electrode attached to a
[32:56] patient's finger the patient was
[32:58] undergoing an OP I believe it might be
[33:00] illegal to do these operations now they
[33:03] have to be done a different way but the
[33:05] patient was uh having an operation on
[33:08] the brain which uh meant that the brain
[33:11] was was revealed and uh during this
[33:15] operation uh the patient had given uh
[33:18] the
[33:19] experimental permission to do an
[33:21] experiment at the same time so the
[33:24] experiment involved stimulating the
[33:25] finger and then uh you can see at the
[33:29] top the stimulation of the finger is
[33:30] that little vertical line um and the you
[33:34] can also stimulate a part of the brain
[33:36] which was concerned with uh uh um
[33:41] sensoring me sensing what has happened
[33:43] to the finger now you can measure
[33:48] uh the the
[33:51] uh the the brain stimulation sorry uh
[33:56] have to remember what my picture is been
[33:59] the um
[34:01] the the finger stimulation is that
[34:03] vertical line and there is a a fast
[34:06] moving clock in the room and the patient
[34:08] looks at the clock and tries to uh say
[34:11] whether the finger stimulation took
[34:13] place at a certain moment and it is
[34:16] pretty well simultaneous just very
[34:18] slightly tiny immense almost
[34:21] simultaneous with the um stimulation of
[34:24] the finger but then that's looking at
[34:26] the fast moving clock
[34:28] and you all it means that the sensation
[34:31] of the finger is judged as being
[34:35] simultaneously simultaneous with the
[34:37] sensation of where the hand of the clock
[34:38] was but that is seems to be almost
[34:41] simultaneous now if you stimulate the
[34:43] brain that's the second line there and
[34:46] that's the wiggly line stimulation of
[34:48] the brain there is nothing felt by the
[34:50] patient until about uh I think it's a
[34:55] half a second a quarter of a second
[34:57] later I can't remember no nothing is
[35:00] felt sorry nothing is felt until half a
[35:03] second later that's the third line down
[35:06] so the
[35:08] the stimulation of the brain is felt but
[35:11] about half a second later then the the
[35:14] next line down that's the fourth line
[35:16] down if you stimulate the finger first
[35:19] then this is the Curious one because the
[35:22] brain stimulation although it was later
[35:25] seems somehow seems to cancel out the
[35:27] finger s imulation even though
[35:29] stimulation seems to be simultaneously
[35:32] with with what the flock said so how is
[35:35] it that the
[35:37] uh later stimulation of the brain
[35:40] somehow could wipe out something which
[35:41] seemed to have got occurred earlier but
[35:44] that's a puzzling thing and I remember
[35:47] worrying about this that maybe one's
[35:49] stimul you one's conscious experiences
[35:53] could be delayed something by something
[35:55] like half a second or something like
[35:56] that uh but then you have to worry about
[35:59] things like if somebody's playing
[36:01] pingpong or well I used to play ping
[36:03] pong when I was at University and it
[36:06] seemed to me if I was going to decide
[36:08] whether to hit the ball one or one way
[36:12] or the other that depended on looking at
[36:13] what I thought the P the my opponent was
[36:16] doing and whether it would my opponent
[36:18] be
[36:20] unex more expecting the thing to go one
[36:23] way or the other then I'd flick it the
[36:24] other way now the current view is that's
[36:27] all done on iously and I said no I was
[36:29] thinking which which way I did that
[36:31] conscious thinking about but somehow it
[36:33] seems to be that this conscious
[36:36] Impressions go are backwards referred
[36:40] now the question is can you make sense
[36:41] of all this in such a way that you if if
[36:46] uh the collapse of the wave function is
[36:48] what's involved in
[36:50] the
[36:52] um the choice I mean that's the view
[36:55] which we have in or the or proposal is
[36:59] that it is the collapse of the wave
[37:00] function which
[37:03] is involves in making a conscious
[37:07] decision then that would have to be
[37:10] something where you you study how the
[37:13] collapse of Wun works and it has this
[37:15] intrinsic retroactive Co aspect to it
[37:18] you have to be careful that it doesn't
[37:20] uh cause causal Loops which which are
[37:22] inconsistent but nevertheless if it's
[37:25] not causing some kind of inconsistency
[37:28] like that you might explain in some way
[37:31] how effects can be retrocausal in this
[37:33] strange kind of way I think that uh
[37:37] Stuart has some certain ideas about this
[37:39] which struck me as quite plausible and
[37:42] the idea is if you have a athlete not
[37:45] just me playing playing ping pong I'm
[37:46] not an athlete but but if you imagine a
[37:49] real professional then um deciding
[37:52] whether say a tennis player deciding
[37:54] whether to hit the ball down the line or
[37:55] crosscourt then that decision
[37:59] uh all the muscle movements and exactly
[38:02] what to do must clearly be unconscious
[38:05] because in order to tip the ball to the
[38:07] left the the player doesn't decide which
[38:09] muscle to move in which exact way all
[38:11] that thing is done unconsciously sure
[38:14] but the actual decision is to whether to
[38:16] make one choice or another that could
[38:19] could be a conscious de decision which
[38:22] is somehow retr causally in this way
[38:25] goes back effectively in time as long as
[38:29] it doesn't cause a causal problem that's
[38:33] okay now argument I was making before
[38:36] about um free will see free will I often
[38:40] wondered about you know doesn't mean
[38:41] anything to say you have free will or
[38:43] something now free will I remember used
[38:46] to play my younger brother at this paper
[38:48] Stone and scissors kind of thing and I
[38:50] got very alarmed because he used to be
[38:52] able to beat me almost consistently and
[38:54] I thought look I'm trying to be as
[38:56] random as I can how can he beat me
[38:58] consistently so what I did is I went
[39:00] into my father's study and I took out a
[39:03] um volume of logarithms and I took
[39:07] opened it in the middle of the p and
[39:09] then I made a sort of Random from from
[39:12] these logarithms taking as basically
[39:14] random numbers I could code which I
[39:17] which I did scissor stone or paper and I
[39:21] just made a long strip of paper and I
[39:23] followed this which seemed to be pretty
[39:25] well random and then I broke e my
[39:28] brother couldn't beat me if I was doing
[39:30] something which is effectively random
[39:32] course it's not random just log log
[39:35] think tables but was effectively right
[39:39] um but the thing was that he could
[39:41] recognize patterns in what I was doing
[39:44] and I was trying to be as random as I
[39:46] could so the argument I'm trying to make
[39:48] here is that it's not Consciousness if
[39:52] it's doing something which
[39:54] is um based on on the collapse of a wave
[39:57] function
[39:58] it has to be something which is not
[40:00] random something Beyond random in some
[40:02] sense it's something which may involve
[40:05] Quantum Realties which are not random
[40:08] and that's way way beyond anything we
[40:10] can think of now and certainly when you
[40:12] think of making a conscious decision the
[40:15] whole point of it is that you go back to
[40:17] decide whether it's a good idea or not
[40:19] to make that decision unless you're
[40:21] trying to be random of course but if
[40:24] it's something which might be beneficial
[40:26] to do a r than b
[40:28] then you have reason to believe this and
[40:30] it comes from your conscious
[40:32] understanding of whether it's a good
[40:33] thing to do or not that's the trying the
[40:36] argument I'm trying to say conscious
[40:39] understanding is something which
[40:40] involves the collapse of the wave
[40:42] function in some Theory which we don't
[40:45] have yet I regard this as one of the big
[40:47] challenges of physics to find a theory
[40:50] and it's clearly going to be very
[40:52] strange kind of theory which involves
[40:54] the kind of
[40:55] retrocausality nevertheless Theory which
[40:58] somehow involves gravity at the same
[41:00] sense times quantum mechanics it's not
[41:03] quantum gravity because quantum gravity
[41:06] means applying quantum mechanics to
[41:08] gravity it's graviti quantum mechanics
[41:12] and so far I think nobody has got very
[41:14] far with that at all and I'll have to
[41:17] leave you with that one thank you very
[41:20] much