Message #499
From: David Smith <djs314djs314@yahoo.com>
Subject: [MC4D] Re: Magic120Cell Realized
Date: Wed, 07 May 2008 05:24:01 -0000
Hi everyone,
I have just finished calculating an upper bound for the number
of permutations of the 120-Cell. To establish it is the exact answer
(which I am virtually certain of), we will have to find a number
of algorithms which I will describe in my explanation.
The calculation was only difficult in one aspect, namely the
possible orientations of the corners. Here is the upper bound:
(600!/2)*(1200!/2)*(720!/2)*((2^720)/2)*((6^1200)/2)*((12^600)/3)
To answer Roice’s question, I did find an arbitrary-precision
calculator (Googol+, trial version) that displays the entire
number in its full glory:
23435018363697222779126210606140343600982219866708667227704291465940007
37743198001537086016413748065359228217622633869330769129523601891497799
90823414733250819032377663096727895392891107724676361939174468537213471
84699260131924584724938945790242680862147295113762851571432130901040238
96149551266842769465158629370618815995041314328829732432057176063611161
23422302770133676753359134856348612503635674252607065815753807941966366
98057536512196715919594180779891338303538085006270891583549467992567391
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43170816415770010483963217284920963354265992129473309221874222731561178
16542353296798264919536869373254412130565886195935986667368898349834998
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68437995628528234082912911481312451144148067422323644080656449490476178
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90453613626399014292854794414276344511148330328685197189376868495672292
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66616881593787942961115669105927538622586908510205223079160329890976613
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71854373062622155659107585797616686931874970164036381491924856162327083
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90715982378923238819174377671246115948128333247228319128499096287090364
06418925007261761200623236257957747401814104819201322380783299932882694
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29742915483006071654290990776376332377597123229369363319211034520828156
16383626599751692734054125142693424208441259140739967321942103460390485
73512549204538199361441602981588922796564372729802637150967463996220269
92509662606254579651749991204772662937610983604733514590588466763484779
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35107696623982892463214959186113390887996406714662349935032809366747705
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13427043475236100473238801150143720068671986307968791851735260237830993
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51846977682603655222729137145829356583863818649600000000000000000000000
00000000000000000000000000000000000000000000000000000000000000000000000
00000000000000000000000000000000000000000000000000000000000000000000000
00000000000000000000000000000000000000000000000000000000000000000000000
00000000000000000000000000000000000000000000000000000000000000000000000
00000000000000000000000000000000000000000000000000000000000000000000000
00000000000000000000000000000000000000000000000000000000000000000000000
00000000000000000000000000000000000000000000000000000000000000000000000
00000000000000000000000000000000000000000000000000000000000000000000000
000000000000000000000000000000000
What a number!
Here is an outline of how I derived this upper bound:
First of all, we can count that the 120-Cell has 120
1-colored immobile center pieces, 720 2-colored pieces
(120*12/2), 1200 3-colored pieces (120*30/3), and 600
4-colored pieces (120*20/4). When a dodecahedral face
rotates, there are 2 5-cycles of the 2-colored pieces,
6 5-cycles of the 3-colored pieces, and 4 5-cycles of
the 4-colored pieces. Since 5-cycles are even permutations,
all permutations of each type of piece (including facelets),
will be even.
Therefore, the 720 2-coloreds can be permuted
720!/2 ways, dividing by 2 because of the even parity.
Similarly, the 3-coloreds and 4-coloreds can be permuted
1200!/2 and 600!/2 ways, respectively. Multiplying
these three terms together, we obtain an upper bound
for the number of ways the pieces can be permuted without
regards to orientation:
(600!/2)*(1200!/2)*(720!/2)
To show this number is exact, we will have to find 3 algorithms:
one that performs a 3-cycle of any three 2-coloreds without
affecting any other 2-coloreds, a 3-cycle of any three 3-coloreds
without affecting any other 3-coloreds, and a 3-cycle of any
three 4-coloreds without affecting any other 4-coloreds. These
three algorithms, when combined with each other and conjugates
(setup moves), can produce any possible permutation of the
pieces.
Now for the orientations. Since the facelets also undergo
5-cycles, all orientations will be limited to even permutations
of facelets.
Therefore 719 2-coloreds can be oriented in any of 2 ways each,
but the last will be determined by the others because of the
even parity. This results in
(2^720)/2
or 2^719 ways of orienting the 2-coloreds. To show
this number is exact, we must find an algorithm that
flips two 2-colored pieces without affecting the others.
For the 3-coloreds and 4-coloreds, I followed closely
the methods of Keane and Kamack in their paper,
"The Rubik Tesseract", modifying their arguments as neccesary
to apply them to the 120-Cell.
Any 3-colored piece can be oriented in 6 different ways.
(not three, because in four dimensions we can reflect
3-colored pieces as well as twist them!) Notice that a
twist (a 3-cycle of the facelets on that piece) is an even
permutation, while a reflection (a 2-cycle of two of the
facelets on that piece) is an odd permutation. Since the
total parity of all of the 3-coloreds must be even,
the first 1199 3-coloreds can be oriented in 6 ways each,
while the last can be oriented in only 3. (If the first
1199 3-coloreds total to an even permutation, the last
3-colored must be one of the 3 even twists, while if
they total to an odd permutation, the last 3-colored
must be one of the 3 odd reflections) This gives a total
of
(6^1200)/2
or (6^1199)*3 ways of orienting the 3-colored pieces.
To show this number is exact, we must find an algorithm
that twists one 3-colored piece without affecting the others,
and an algorithm that reflects two 3-colored pieces without
affecting the others.
Finally, the toughest part. The orientation of the 4-coloreds
required me to generalize the group theory based solution for
the corners of the 3^4 cube by Keane and Kamack to the
120-Cell.
In their paper, Keane and Kamack first describe that any
particular 4-colored piece can never be in an odd permutation
of its facelets, because the 4-coloreds split into two
different groups: the even and odd permutations, which
happen to be mirror images of each other. This rule applies
equally well to the 120-Cell.
Hence, each 4-colored piece can only be oriented in 12 ways.
(4!/2) There is an additional constraint. In their paper,
Keane and Kamack show that the orientations of 4-colored
pieces in 4D space, which form the alternating group A4,
can be divided into three sets. They describe orientations
using cycle notation of the four faces, labeled a, b, c,
and d. The subgroup N consists of the identity permutation,
(ab)(cd), (ac)(bd), and (ad)(bc). The subgroup S consists
of (abc), (adb), (acd), and (bdc). The subgroup Z
consists of (acb), abd), (adc), and (bcd).
The authors then show that the group of these three subgroups
is isomorphic to (the same as) the group of residue classes,
mod 3, with N as the identity. This means that we can assign
the number 0 to N, the number 1 to S, and the number -1 to Z,
and adding these numbers mod 3 is the same as taking the product
of elements of these three subgroups.
Notice that this entire argument applies equally well to
the 120-Cell as to the tesseract. Now the only thing left
to show is that the sum of the orientations of the 4-coloreds
(counting 0 for an orientation in N, etc.) mod 3 is always the
same, whether to the tesseract or the 120-Cell.
The orientations can be defined by assigning, to each 4-colored
piece, a letter to each facelet and each position of each
facelet. Then each orientation can be described by a 4-letter
string (e.g. ABCD) relative to the position it is occupying.
When pieces or cubies rotate in a cycle, their facelets undergo
n seperate cycles if they have n facelets. The important thing
is that there are always n disjoint cycles. In the tesseract,
every corner rotation boils down to four 4-cycles of facelets
for each cycle of four cubies. In the 120-Cell, it is the same
except it is four 5-cycles. If we can show that in
cycles of any length, the sum of the orientations of the pieces
does not change, we will have proved this for both the tesseract
and the 120-Cell.
Consider four 2-cycles:
ABCD 1
ABCD 2
Each row represents a 4-colored piece. The actual 4-cycles
are vertical in direction. For example:
ABCD 1
CDAB 2
This means that facelet A goes where facelet C was, etc.
In this example, piece 1 performed an N-twist. Now notice
that since we are dealing with 4-cycles, the facelets of
piece 2 must return to the original positions of the facelets
of piece 1. Therefore, piece 2 also performed an N-twist.
It can be checked that if piece 1 performs a Z-twist, piece
2 performs an S-twist, and if piece 1 performs an S-twist,
piece 2 performs a Z-twist. Therefore, the sum of the values
does not change. (N=0, Z=-1, S=1)
Now we can do a proof by induction to show that any four
cycles has this property. Assume that 4 k-cycles always sum
to the same amount:
ABCD
.
.
.
ABCD (not neccesarily this orientation)
Adding another piece, we are in the same position as before.
If the next-to-last piece is an N-twist when moving to the
position of the last piece, then the last piece must also
be an N-twist when moving to the position of the first piece
(since the ends of the cycles must return to their original
locations) Also, a Z-twist implies an S-twist and
an S-twist implies a Z-twist.
Therefore, no matter what the length of the cycles, the
sum of the values of the orientations never change. This
means it is true for both the tesseract and the 120-Cell.
So now we know the sums of the orientations, mod 3, never
change in the 120-Cell. Since an N-twist is 0, we can have
an isolated N-twist without affecting any other pieces.
The value S - Z must therefore be congruent to 0, mod 3.
This means that the first 599 4-colored pieces can
each be in any of 12 orientations. If the value of orientations
up to that point is 0, the remaining value must be an N-twist.
If it is 1, the remaining value must be a Z-twist, and if
it is -1, the remaing value must be an S-twist. In each case
there are four possible orientations left for the last
4-colored piece. Therefore, the upper bound for the orientations
of the 4-colored pieces is
(12^600)/3
or (12^599)*4. To prove this is exact, we must find algorithms
that show that any N-twist can be performed without affecting
the rest of the pieces, and algorithms showing that any Z-twist
can be performed along with any S-twist without affecting any
other pieces.
When we multiply these figures with the ones for permutations,
we arrive at the final answer. I sincerely hope that I did not
bother anyone by writing this very long post. I just wanted to
share my results with those that are interested.
I am not worried about finding all of the algorithms to make
this figure exact. They will probably arise naturally as we
play with Roice’s program.
I want to once again thank the members of this group for
helping me, and for putting up with my long posts!
Best Regards,
David
— In 4D_Cubing@yahoogroups.com, "Roice Nelson" <roice3@…> wrote:
>
> Awesome, I didn’t want to ask directly, but I’m excited to hear of
your
> interest in looking into the problem of the number of permutations!
I
> wonder if this particular calculation has ever been done before.
Also, I’ve
> seen and used big number calculators on the web before, so I also
had to
> wonder how easy it would be to find one that would be able to show
all the
> digits in the final answer to this problem. I hope one is out there.
>
> cya,
> Roice