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C~pyri t Igp?, by PIbICx?lOU U n i d l y
second Printing 198
Third Prinfiog I
Founh hindcg I
Fifth PIbIlilIg 1966
Rinted in the United S t a t a hmk
PREFACE
AND BIlBLIOGMPHICAL REMARKS
S T R ~ Grom the me w ha t vague notion
of symmetry harmony of pmportkns,
these four lecture8 gradually dGvdop irst the
goomebic concept of symmetry in its sever l
forms, as bilateral h'analatory, rotati
ornamental and erysrallographic symmetry
etc, andy
ise to the general deaunder-
lying all these special Forms namely that of
invariance of a umfqumtion elements
under 4 group o automorphic ta*-tions. 1aimattwotbinga:ontheonthand
to diil ay the g ~ tariety of applications
of the priaciple of symm try in the arts in
inoipnic and org nic nature, on the o t k
hand to cl rify step by step the philmophieo-
mathematical dgnhhnce of the idca of pym-
metry. The IsWw purpose m kes it neots-nary to wnfmnt the notions and theorLen of
symmetry and relativity, while numerow
illustrations supgmrting the text hdp to
accomplish the former.
s readersof this bouJt I had a wider circle
in mind than that of leacud speeialista It
does not shun nathematiw that would defeat
its purpose), but daailed treatment of mwt
o the problems it deals with in p rticul rbomplete rnatbnatical treatment, is beyond
its scope. To the lectures, which reproduce
in slightly d i e d ersion the Louis lark
Vanuxan Lectuns given by the author at
rinceton University in February 1951, tw
appendices eontaiaing mathematical proofs
have been added.
Other books in the field, as for instanceF. aeger's daasical ecttacs on th p r i ~ I e
8/13/2019 Symmetry by Weyl
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o ym y and its a icutims in natural m i m e
(Amsterdam and Lwdon 1917), or the
much smaller and r ore recent booklet by
Jacque N La p E at su applicatim(Paris, Albin Michtl, 1950) cover only part
of the mate though in a mom detailed
fathion, Symmetry is but a W i e n
D A q Thompson s magni6-t work 8
Orour off m New edition, Cambridge
En@. and New York, 1948). Andma
Speiads Tkmis ar ru~panuan sndliukrOrvlnuffg (3. A d . Berlin 1937) and other
publieatiom by the same author an mpor-tant for the synopb of the aesthetic and
mathematical sw of the subject JayHambidge s D ic . pm d t ~ Yale Uni-
versity Prrsq 1920) has little more th n he
name n commonwith th present book. Itsclosest dative is perhaps theJuly 1949 num-
b on symmetry of the Ge-rman periodicalSrudim awde( I., pp. 203-278: q u d
as .stuU?rn G%iMrnl ).
A comple-te Iist of m- for the ilhrstra
tions is to be found at th end of the book
To the Frh-ton University reaa nd ts
editorsIwiahtoexpreaswarm~foathe
inward and outward carethey have lavished
on this little volume; to the authoridea of
Rineeton Univasity no less Bincen thadksfor the oppochmity they gave me to deliver
thkswansongonthee-veofmyrerinment
from the Institute for Advanced Study.
5zemMmw~nzDs nrb 7W
CONTENTS
Bilateral sym~~etry 3
Translatory, rotational, and related
symmetries 4
Ornamental symmetry 83
Crystals. The general mathematicalidea of symmetry I 9
PPENDICES
A. Determination of a l l finite groups
of proper rotations in g-space 49
B Inclusion of improper rotations IS5
Acknowledgments in
Index 6
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IUTER L SYMMETRY
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BILATERAL SYMMETRY
IQ I A M N Q P M I S T A K E N ~ ~ C ~ ~ ~ ~
used inoureverydaylanguageintwomean-
ings. In the one smse syqmetrie meanssomething like well-propwtioned, well-bal-anced, and symmetry denotes thatWI? ofam-
d a n c e of several partr bywhich theyhte
grate into a whole. Bmty is bound upwith
symmetry. Thus Polyklcitos, who wrote a
book on proportton and whomthe
ancientspraised for the harmoniow perfeetion of his
wdptum, uses the word, nd UIWfollow
him in setting down a canon of proportions
for thehuman figrm1 In this the idea
is by no means restricted to apatial objcns;
thesynonym harmony pointsmoretoward
its coustic l andmusical th n ts geom
I pplications. h m s a good German
q u i d e a t for the Greek symmetry; for like
this t carries also the emmotationof middle
'D u, V i iBi hn mn r n e n d k k Anpwrias 1528.Tobcaraa,D%uhimrltdoanotiratlxword
Igmmehy, but the a&u&d'' Latin tran*lthnby
Ida M a dJoachb Camemdu~1592) beam thc t tk
t k ~ p l r r i r r r r T o ~ t c 8 t h e s t s t c m e n t l a.aaibcd 4Mc.ml&u, wp3) tbat rJm empbymmt
a p t many ntnnba would almost esgm er
c o r r s m a i n l e u t p a n r S e e * ~ b a f ~ A usuja dc 1 mppwph dmu DiOdOIT 4 98
5-9 fn Cbuiqm 26 1951), pp. 63 66.
Vibuviua d c h 'sSpmcuy NRUp q m
tion RDportionirthcmmmcnamtitiondthc
variow d m e n t pam with the whdr For a
marclaboratemDdanattcmptintheaame~
k CCOt 8G David Bkk l d Aeuwlie ln8asUI4, am-
bridgqU,HmvdUnivaaityReas 1933,andthelcchmrbgtheaamelllthorm Amamrmatieal
theap of aatktb llld it a*tioIla to pomgand mu&, ics u t i w Pm &t, Vol. 19 (July,
1932). pp 189 942
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measure))) th mean toward which the
virtuous should strive in their actions accord-
ing to Aristotle's Nicomachean Ethics, and
which Galen in De &mpatmmtix d d b e s
as hat stateofmind which isequally removed
from both exaemes: w W p o v rrp ~ ~ 6 7 b
TGV U ~ VW x e ~ .The image of th balance provides a
naturallinktothesecondsenseinwhichthe
word symrn hy is used in modern time8:
bilata.l spnwly th thesymmetry of left and
right, which isa ow~picuousn th structure
of the higher anLnaLs especially th human
body. Now this bilateral symmetry is a
strictly geometric and, in contrast to th
vague notion of symmetry d k c d Maran absolutely pr concept. body, a
spatial codgumtion is eymmetric with re-
spect to a given pknc E if it is d e d nto
itself by reflection in E. Take any line 1p
pmdieular to E and any point p on t there
Qdas one and only one point 8 on I which
has th same dhtance from E but lies on the
other aide. The pointp' coincideswithp ody
ifp is on E. Reflectionin E is that mapping
FIG. 1
R in E.
of space upon it , S: p +p , that carries
thearbimrypointpinmthisitsmirrOrimage
p' with rrspect to E. mapping is defined
w h~ e ve r hlle isestablishedby which every
point p is associated with an image '. An-
other example: a rutation a d papen-dicularaxk, say by30°,camiesBachpodntp
of sp ce into a point p and thus deb- a
mapping. figurehas rota- symme*
m u d anaxislifitiscarriedintoitrdfby
ll rotations m d . B i l a d symmetry
a p p m thus as the int of a geometricwncq?t of symmetry that m to aueh
operations as relkdons or rotations. Be
came of their omnplete rota- wthednleintheplane,thesphdeinspace
were amsidered by the the
most perfect geometric f i p e s , and Asktotle
asaibedsphaicalshapetotheeeleatialhodies
becauseanyotherwoulddctcaetfromthcir
heavenly perfection. It L n this tradition
that a.modem pxt edQesses th Divine
B d n g a s ' T h o u g r e a t ~ :
a hgr.6otmeW f m ~ o i hglustinns
Frmn wbum my som*os ,Fa dl 8It8fn' tamdrEcgsTI b pmt in sha drFs q s
G ~ J ~ ~ E B M ~ Q E ~ ~ .
S ymm e a y , a s w i d e o r a s ~ w a a y o um a ydeflneitsmewing s one dea by which man
throughtheagabastriedto compreheddand
createorder, beauty, and perfection.
T h e c o u r a t h ~ ~ e l e c t u n s w i l l ~ i s a s
follows. P i w ll d i i ilateral sym-
metry in some detail and its mle in art as
* A ~ u a W i o L h a m , ~ ~ f i m mk-
pony, Hamurr, B ~ ~ G undCb. 1 ~ 1 .
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well asorganic and inorganic nature. Then
we shall generalize this concept gtadually,
in the direction indited by our example of
rotational symmetry, irst staying within the
d e s geometry, but then going bqrond
th s limits through the pmxs o mathe-
matical abstraction along a road that will
y ead us to a mathematical idea of
peat generality, the Platonic idea as it were
behind l l the speci l appearances and ap-
plications of symmetry. To a certain degree
this scheme ia typical for ll theoretic Lnowl-edge: We begin with some general but vague
principle symmetry in the first sense , then
find an important case where we c n give
that notion a concrete precise meaning bi-
lateral symmetry), and £ru that c se wegradually riae again to generality, guided
more by mathematical mmu tion and
abstractionthan by themiragenof philasophy;
and ifwe re lucky we end up with an idea
no less universal than the ane from which we
started. Gone may emuch of its emotional
appeal, but it has the same or even greater
unifying power in the realm of thought and
h exact instead of vague.
open the discussion on bilateral sym-
metry by using this noble Greek sculpturefmm the fourth century B.c. the statue of a
praying boy Fig. 2 , to let you feel as in a
symbol th great significance of this type of
symmetry bothfor life and art. Onemay sk
whether the acsthetickalue of symmetry de-
pends on its vital value: Did the arrist din
cover the symm try with which nature ac-
cording to some inherent law haa endowed
its creatures, and then copied and p e t f d
what nature presented but in imperfect
r d k a t i o ~ ~ r haa the aesthetic value of
symmetry an independent source I am in-
FIG 2
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dined to think with Plato that the mathe-
matical id- is tho o G m rigin both:the mathematical laws govaning nature re
the ori in of apm y in nature the in
t u i t i v c ~ t i o n o f ~ i d e a i n t h e ~ d v es m i n d i t a E l r i g i n i n a r t , ~ I a m
ready to +t that lte arts the fact he
bilateral symmetry of rhe human body in ita
outward appsaranee bas cted as an addi-
t i o n a l ~ ~ ~
ofallandtnt~theSutnerians rm
to have been pgrdhll lrty fond to d strict bilateralmheFatdiesgmmerry. A t v p i d d b
~onthefam0rmEilvervaaofKin~En-
temena,*rukdinthedtgdr;lgash
FIG
around 2700 B.c. shows a lion-headed eagle
with spreadwings ace, each whose clawsgrip8 a stag in side view, which in its turn is
frontally attacked by a lion (the stags in the
upper design are replaced by goats in the
Iowa) (Fig. 3). Extension of he exactsym
metry of the eagle to the other beasts ob-
viously enforces their duplication. Not much
later the eagle is given tw heads facing in
either direction, the formal principle ofsym
metry thua completely overwhelming th
imitative principle of aud m nature. This
heraldic design can then be followed toPersia, Syria, later to Byzantium, and anyone
who lived before the First World War will
remember the double-headed eagle in the
coats-of-arms of ~ z a k s tRussia and the
Austm-Hungarian monarchy.
Look now at this Sumerian picture Fig.4 .
The two eagle-headed men are nearly but
not quite symmetric; why not? In plane
geometry reflection in a vertical line can
lso be bmught about by rotating the plane
in space around the xis by 180. If you
look at their rms you would say these two
FIG
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monsters rise from each other by such rota-
tion; th overlappings depicting their@
tion n spaceprevent the plane picture fromhaving bilateral symmetry. Yet the artist
aimed at t symmetry by giving both
figures a half turn toward the o h e z and
also by the arrangement of feet and wings:
the droopii wing is the right one in the
left fiseun. the left one in the right figme.
im designs on the cyhdriwl Ba b y l w h
se l stmles are frequently ruled by -die
symmetry. I member seeing in thedh
tion of my form r coihgue the l te Emst
Henfad, samples where for m w ' s lre
not the head, but the lower bull-shaped part
of a god's body, rendered in p f i l e , w s
doubled and given four instead of two hind
legs I n c h r i a t i a n t im e s o n em yw e a nanaIogy in c rt in qnwmtations of tf
Eu a s on Byaantiae patsn Fig.5 ) , w h e m t ~ m ~ p ~ m C h r i s F s @ f a d D gthe disciples. But here symm y id not
~eteandbaadeady-thanfarmal
f o r C t a s i s t o n o n e s i d e ~t brard,ontheorherpomsthewlne.
Betwen Snmeria and Bymmiwn let meins t P A hese n mled s (Fig.
6)arefiomDmius'palaeeihguSab~ilti~
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thedays o Marathon. h d n g he
we find them hr -H Fig,7) at theMegaron in Tiryns, late h dic about 1200
3 0 Who elieves strongly in tristoric e m
tindty and d q ~ d c n e t in trace the gr80b
tl desigss o e life, dolphin and
o c t o p u s , b i c k t o ~ M i n ~ t n c u l t u r e o f ~
the hg ldio symmeay to oriental, in the
last .hstancc Summisn, htlumm Skip
t h ~ o f f l c a t s w e s t i l l s t e t h e s am c i n f l u -enceaatworkinthkplaque~i. )fromthe
altar en hute in the dom o T d 4Idy, leventh century A.D. The peawdw
drin ingfrom a pine well amongvlne leave
a r e a n a n d i e n t C l d t b s y m b d d b
ralitp the t h e a l dk symmetry is
Oric~tat
For in contrast to the orient, occidental
art, like life itself, is inclined to mitigate, to
I w m , to modify, even to break strict s v -
metry. But seldom s asymmetry merely the
absence of symmetry. Even in asymmetric
designs one feels symmetry as the norm from
which one deviates under the influence of
forees o uon-formal character. I think the
riders from the famous Etruscan Tomb of the
Triclinium at Corneto (Fig. 9 pmvide a good
example. I have already mentioned repre-
sentationsof the Eucharist with Christ dupli-
cated handing out bread and wine. The
central gmup, Mary M e d by two angels,
in t is mosaic of the Lord s Ascension (Fig.
10 in the cathedral at Monreale, Sicily
(twelfth century), has almost perfeet sym-
metry. [The band omammt's above and
below the mosaic will demand our attention
in the second lecture.] The principle of
symmetry is somewhat less strictly observed
in an earlier mosaic from San ApoUinare in
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Ra- Fig. I , siwwin i wmundcdbyanan~guardoflnmor. ForlnnanceMaryintheMmvealemossicr?liees
b a t h h e n d s ~ y h t h e o r o r m r s g e s -tme;hrrconlytherigbhandsanraiad-tt~ h s made f rther into ds in thenext picture Fig. 12 , a yzanfhe relief
ikon fromSanMar- Venice. It is ahi? ?,and o cmm the tw figwen praying foxmercy s the Lord s about to pronounce the
last judgment cannot be mirror im ge o
e cb other;for to the right st nds hisV i
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uem1y we touch &round hem w h a s the
p.eci.c gBOrn @ of Gitatgal sym-
m e t r y b G g i a s l t o ~ ~ ~ ~ € h e v a g u e w t i o n
o A ~ d G s i p p w i f h *
w started. SymmGPrp.3 w Dagt)$atF r e y i E , a n ~ O n ~ . d ~ i nI b t , ~ ' ~ ~ n s t a n d ~ ~motionand awmhg, the me order aad law,
the other arbitdmssand aeddtitt, the~ ~ ~ i y a a d ~ t h e ~ ~ l i f c ip I a y a s d U . ' wkamecGalor-
are r e p m a d as symbols for wm s h o r ~ d r a y s w g i v c ~ l i n h e y r a -l e viaw not inp . ohablyl o a ~ E e a a o n s p * ~ d~ d ~ , w ~ l t h c y ~ ~ ~ -
~ p l e s o r ~ ~ a n d ~ a t e ,rn bila* nymm@ic t is, hw-r>p u e t k t n o t ~ ~ t l y h ~omas o
God&catbdra ared&rent, asforinst nce
inc2ePms. ButinpFad*every-~ ~ ~ e e m s t o d ~ b o t 1 3 C ~ C C t h ecathefltai,dyto*factthat*-
were built io dWerent pesiadk It is unda
standable&at a rttrr imewasno1ong.bsatis
& d w i t h * ~ o f a n w t i b ~ ~ ~ ~o n e m a y ~ b n e o f ~ a r y r r z m c t r -
M i f i m h a g e a o c c n r w e r c : r h e r c i s a ~ ,b e i r a f a r k a d e & g r r ~ o t a ~~ i n t o w h k h a ~ ~ .aturea s d a a p a i n t e n l a a L c u s t e B ~ m o t i f . 1~ ~ w i l l ~ y h ~ n r e t o y o o ~ ~
T e ~ ~ ~ ~ f a m i I E B T t o n w j ~ * I k e La t i t i a m y e . t u d - e % r y d a y , i a W ~ -
ofsilaapkuur.~ w e a r e a h D u t t o ~ o a a M T O a
natart, 1st m
eanside whatphilo~& I iu right. To the adareas fihunk p. 276.
mind them is no innerdiikmx no polarity
betweenleftand right, a s t h e m i s i s f o r ~
inthecontrast~matcand mak,orofthe
ant& aod p d o r nds aaanimal. Itreq an arbitrary act of choice to detar-
mine what is left a d what is right Butafter it ia made for one body it is
for every body. I must ixy to make this alittle clearer. In space the distinction o left
;andright eon- the orientation ofa screw.
IfyouspeakofturningIeftyoumeantbatthe
s n in which you turn eombined with the
upward dire tion from foot to had o you~
body forms a left screw. The daily rotationofthe earthtqetherwiththeMondits
axis&om South to North Pole isa left scrav,
it i a right saew if you give the ash €he
opposite W t ion . Therearecertaincrystab
line substanca called optically active which
betray theinnerasymmea~f theird t u -
tion by turning €he pohmatm.
plane ofp o k h d light sent through them to
thel a~totiaGright;bythia,of-,we
meank t hesut c nwhichtheplane-tea
while the l travels in a definite diredon
combined with that forms a left
a e r e w ( o r a r i g h t e n e , a a t h e e a s e m a y b e ) .H e n c e w h m w e a a i d a b a r e ~ n o w r e p c a t
in a t e m h h g y due to Lei-, that left
a n d r i g h t a n i m b m i * w e m t t o ~
thattheinnershuchlreofspacedoennot
p s m i t w , e r w p t b y a r ~ C h o i e q m d i a -
tingukhaleftfmmarightm
I wish to make tbis und-tal mrtienstill
more preoise for on it depends the entire
theory of d v i t y which is but
v t f symmary ceding to Eudidone can describe the s t . f apace. by anumber of basic relatiom between points
such aa ABC ie on a straight line, ABCD lie
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in a plane AB iscongruentCD Perhapsthe
aat way of dacribing the spucture of spa
is the one Hehnhdtz adopted: by the singln&Oll of COBpWU ofm A Dapp@ S
of space d t e s ith every point a point
pl:p +pf. A pair of mappings S Sf:@-+d,
~'+p,ofdchtheoneistheinvera~ofthe
other, so that if S c rries p into p then Sf
FIG 13
~ p f b a i n t o p a a d p i o G v ~sof as a pair ofo~lb$o-memappings or imcrp
fanrarions A ~ ~ t i o o . w h i o h ~ ~ ~
thestrue~eof-ifwedefinethisstructuruintheH- way, that
mean that it carriesany tw m w t igurinto two w on& called an d g
m p h by thc ntathema-. dbnie
that thia is the idsa undalyhgthe gemmetric conoqt Mwa u ~ & v j a f i g u r e i a t o t m e f h a t
in mwbnizs .-itife e c h o f t h e n v o ~ i s w d d a a l b y i ~ ~ 'What we mean then by stating thatl t a d
rightareofthesameeostnceistheh~th~r ediar n splaar i s an a&mw hidnn.
Spaceasmichisaudiedbygeom~. But
spaceisalaothemadiumofa~physteaI00
nnrrn The strnenne of the physical
world is rweated by the general laws of na-
ture. They are formulated in temw of cer-
tain bslsic quantities which are functions in
spaceand time. We would d u d e hat the
~hys ical structure of sp ce "contains a
screw, to use a suggestive ftgure of speech, if
these lawsw e ot invariant throughout with
nspect to reflection. Emst Mach ells of heintellectualabockhemeivedwhen hele rnsd
asa boy that a magnetic needle isdeflected in
a cer ainsense to the left o the right, if
suspended pardel to a wire through which
an electric - is sent in a de6nite direc-
tion (Fig. 14 . Since the whde geometricand physical wntiguration, including the
electric current and thcm t h and north poles
of the magnetic needle, to all appearances,
are symmetric with respect to the plane Ehid through the wire and the needle the
needle should react likeBuridan's a s etween
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equal bundles of hay and reluse to decide
betwealeftandright, just as sa ho fe qu al
armswith equal weights neither go down on
their left nor on their right side but stgy
horizontal. But ppe r nces are sometimes
deceptive. Young Mach's dilemm was the
result of a too hasty amamption con-g
the effect of reflection in E o n the dectric
current and the positive and negative mag-
netic poles of the needle: while we knew a
how goometric entities fare under
refloetion, we have to learn from nature howthe physical quantities behave. And this in
what we find: under rdieetion in the plane
theelectriccurrentpreewea its direction,butthe magnetic muth a d orth pdes are nter
changed. Of course thisway out, which re-
estaMishen the equivalenceof eft and rig& in
pmible only becauseof the-tid equality
of positive and negative majl;netism. AU
doubts were d i e d when one found that
themagnetimn oftheneedlehasitsariginin
rmleculardectricc-tseireulating~~)und
the needle's direction; it is dear that
reflection in the plane E such m t s
hange the m e n which they flow.
Thenet t is that in aY physieanothing
has shown up indicating an intrinak diffs-
enceofleftandright. Justasallpointsand
alldire nsinsgaceareeqaivalent, mare
left and right. Position, direetioh lcft and
rightarenlutk-concepts. Inlanguagetirrg dwith theology this ssue of relativieywaa din-
cused at great length in a famousoontmvauy
berwaen bnia and Clarke, the t o
clergyman acting as the spokamau for
NRaton.' ewtonwith his belief n abaolute
stc G w. Lcilrmk, Pidhphi SI* cd.
Oshardt 1875 scq.), w pp. 352-440, in
Lribnil hirdkit8r. 5.
space and time d d w motion a p d
of the creation of the world out of God'sarbitrary will fm o t h d t would be in-
explicable *hy matter moves in t is rather
than in any other d rectton. Leibniz in loath
to burden God with such d & a rm lacksufficientreason. Says he, U n b he as-
swnption that space be somefbing in itself it
in impwible togivea reasonwhy Godshould
have put the bodies (withoutampaingwith
their mutual distances and dative positions)
just at this particular place m d not nomewhem else 6r nstance, why He should not
have arranged everythkg in the opposite
order by turning East and Went about. If,onthGotherhand,spaceisnothingagthan
the spatial ords and relation of things then
the two tea supposed above, the ctu l
one and its transposition,are in no way dif-
ferent from each other and th m lo n it
is a quite inad-ble question to ask why
one srate was pmtared to the other. By
pondering the problem of I& and right b t
was first.led to hia conception of space and
t h e as f s f intuition.s k t ' s opinion
s ms to have en this: If the first creative
act of God had been theformingofaleft
hand then this hand,even
at the time whenit could be wmpated to nothing dsa, d
the d i v e haracter of ft, which can
only intuitively but never conecptually be a p
prehended. Lei- contradicts: Accordingto him it would have made no difference if
Gad had created a right hand first rather
left one. m e must foIlow the
world's creation a step iiarther before a differ-
ence can appear. ad God, rarha than
~ M s ' * K l i t i l r d a r r i n m v ~ ~ & ~
pxiaUy 1 3 o l t h c ~ ~ + e r j ~ i . m ~ mMu @ . .
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making irst a lefr and then a right hand,startad with a right hand and th o f d
another rigat hand,He wm l havech ng d
theplanoftheuniveawaotinthefirstbutinthereoondact,bybFiaBlngforthahandwhich wss equally rather than oppositely
ral to the ht-mated s p e
scientific thinking lea with IAbnk.Myrbiaal W&bg bss always t lrrn the wn-
-view asiserincod by itswageofrightnd ldt ar symbols for nuch pola~pposites
an goodand evil. Younecd d y hin d thedouble m e q d theword ri ht itaelf. In
t h i s ~ f r o r n h d i c h e l a n a a l a ' ~ f ~ C ~ ~ n -tim of dem fFom the S i e dling (Fig.
15) God2@ight h a d , on the right touehea
life into Adam's I .
Pwpk shakt right hands. Sinida is the
L a t i n w d f o r M t , a n d ~ d S p e a l r sof thekftsideoftheshiotdasitasinirapside.
But s n srnrm is at the same time that d o h
isevil,andin~~nmonEngJinhodytbisfigwative - of the Lath ur-
vives.@ Of the r ~ ealefactm who wcre
crudficdwithChrist,theonewb oks*Himtopar*isonHisright.StMatrhm,~hepta5, a d b e s the last judgment as
f 0 l l ~ ~ ~ : A n d t l e s h a l l s e t t h e s h a e p o n B i sright hand but the gQaa on the eft. Then
shall the King ray lmto h m n his right
hand, ome ye, bkmed d my Father, in-h e r i t t h G ~ ~ m ~ h p -thefou~datio~ofdieworkl.. . Theahh ay also unto them on the left hand,
D e p a r t f r o m m e y e e u r s a d i ~ - ~~pnpemtfarthedevilandhisang&.
FIG IS
G ~mmemh~ra~actcne~dnrich-
o n c e d d i ~ i n z u r i e h 0 n ' ~ a n d h e nin painting$'; togemcr with an artkle on
The p b lem d Pvasion b
Rap$ae17stap is try^ mnv find it
print&in&breviatedf&minhis&bbn~ u K i e s h i c h t c , l 9 4 1 . B y a n e d w
amples, ar Raphael's isliw Mabum and
Rembmdt's etching rmaPsrpps Bgifk fh 66
maW6lBin alea to shmv that right in
p a i n t i q h a s a n o t h e r ~ r t t h a n M .Ractieallyallmethods ofrepduction inter-
changelek andright, anditseemthat rormSrtimcsweremuchlemsmsitivethanweare
i n v c d m . E v a Rm~brarrdtdid not hesitate to b&g r Descent f%wmthe me as a converse etcbiug upon the
d e t . Ccmaklechg thatwedo a lotmore
reading than thepeople say, of the
mtury t is suggests the hypoahesis that the
sa
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d i i m c e pointed out byW8lfflinis CO~Ccted
with our habit of reading from left to right.
Asfar as I remember e himselfrejcctedthis
s well as a number of other psychological
explanations put forward in the disc
after his lecture. The printed text concludes
with the remark hat the problem obviously
has deep mots m e hicb reach down to
thevayfoundatiomofour~~~~nature?
I for my par4 m dkidhed to take the
maiter that Saioltsly.'
In &ce the belid in the equiv lence ofleft and right has bem upheld even in the
face of e t in biological facts p-tly to
be mentioned which seem to augge8t theirinequivalence even more strongly than doos
the deviation of the magnetic needle whichshwkd young Mach. The same
of equivalence arises withrcapecftopnstd
fume, which are intedmqed by i n d g
the d ii t i o n of time, and with respect topoJihhw and ncgnlr'w id .In then CaSeq
especially in the second, it is p h a p d-th n for the pair kft-right that a evi-
dence is not m&Xent to settle the qu d o a;
the empirical facts have to be consulted
To be sure the role which past and future
play in our wnsdowwa would inc i tetheir intrinsic difference-the paat knowable
and mcbqeable, the future unknown and
still alterable by decisiom ken n o w 4
one would expect that this difference bas itsbasis in the physical laws of nature. But
t h e awsofwhieh we canboast a reasonably
certainknowledge are invariant with respecta l s ~A ~ a t t a ~ , und knBiide, Amicia, J h h dm 8slnrdkhm GaMa
1926 p.n uliua . schl-, ' ' III~IW alk h a
dd quadri, Ctiticn 28 1930 p. 7 Paul Opp€,
Right and kft in Raphad s cammu, j% bnaI
th W 0 k g nd Courtm II d ,194, p. 82.
to thehvmion of h a they arc withre-
spect to the intaehange of left and rlght
Leibnizmade it clear that tbt emporalmodi
paatandfutuxe&tothecdsftuskmcf
thewwld. ' E v e n i f i t ~ ~ e h t t h e g a o t
-wave laws formulatedby qu emphya r e n o t a l t a e d b y l e t t i n g ~ f i o w b ~
them e t a p h w idea ausation, aod wi th
itthcenewaycharacteroftime,mslyeater
phy through the rtatisieal in
oftlaose laws in rmll ofprobabilitp and
particlea our present physical k n o w
leaves us even lnorr nncatain about theequidcaec or nOn valence of positmand m v e eopidy I tseem di&dt to
devisephysicallawainwhichthaparcnot
iny w but the ne@%tive
part of the positively chargfd proton till re-
mainstobedisawsnd.
This M-phiiomphical excursion was
netdedasabaekgroundhrthetheof
the I&--right symmetry in nature; we had
t o u n d d t h a t t h o m # t i o n
ofnannc posscsai that s w j . &t one
W i U n o t ~ t h a t a n y l l p c d a l ~ n a -tureshowsit to p e r b t h . Evenw itissur-
lnisiag to what eat- it p a i k l?memustbeareas~lfwthiqanditisnotfarto
stek:aatateofequilibriumis~ytobeaytn-metric. More preciacy under conditbna
which dstermint a unique a t e of cquilib-rium the symmetry of th benditions m ft
carryover totheatateof equilibrium. T h e
fore tennis balk and starr arc sphww the
ear thw~bGasphsTe twi f i td idno tro ta te
amuadaaaxis. T h c F a t a ~ ~ i t a t
tbepoles but the o ta r i dw cyhbi cal sym
metry around i&ads s prcscnnd. The fea-
nnc that xplanation is, thacforenot the mtational symmetry ofits shape but
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