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The HOME SECRETARY and the FOREIGN SECRETARY of the ACADEMY

The CHAIRMAN and the PERMANENT SECRETARY of the NATIONAL RESEARCH COUNCIL

WILLIAM DUANE, '23
R. G. HARRISON, '23
J. C. MERRIAM, '23
E. H. MOORE, '23
F. SCHLESINGER, '23
W. M. WHEELER, '23
F. G. COTTRELL
C. E. MCCLUNG

A. L. DAY, '22
GANO DUNN, '22
L. J. HENDERSON, '22
W. J. V. OSTERHOUT, '22
R. M. YERKES, '22
AUGUSTUS TROWBRIDGE
E. B. MATHEWS
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J. M. CLARKE, '21
LUDVIG HEKTOEN, '21
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W. A. NOYES, '21
C. A. ADAMS
G .W. McCoy
F L. RANSOME

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QUATERNIONS AND THEIR GENERALIZATIONS
BY LEONARD EUGENE DICKSON

DEPARTMENT OF MATHEMATICS, UNIVERSITY OF CHICAGO
Read before the Academy, April 26, 1921

1. The discovery of quaternions by W. R. Hamilton in 1843 has led to an extensive theory of linear algebras (or closed systems of hypercomplex numbers) in which the quaternion algebra plays an important rôle. Frobenius' proved that the only real linear associative algebras in which a product is zero only when one factor is zero are the real number system, the ordinary complex number system, and the algebra of real quaternions. A much simpler proof has been given by the writer.2 Later, the writer3 was led to quaternions very naturally by means of the fourparameter continuous group which leaves unaltered each line of a set of rulings on the quadric surface x; + x; + x; + x; = 0.

The object of the present note is to derive the algebra of quaternions and its direct generalizations without assuming the associative or commutative law. I shall obtain this interesting result by two distinct methods.

2. The term field will be employed here to designate any set of ordinary complex numbers which is closed under addition, subtraction, multiplication, and division. Thus all complex numbers form a field, likewise all real numbers, or all rational numbers.

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Just as a couple (a, b) of real numbers defines an ordinary complex number a + bi, where i2 — 1, so also an n-tuple (x1,.., x) of numbers of a field F defines a hypercomplex number

x = x1е1 + x2€2 + .... + xnen,

(1)

where the units e1, en are linearly independent with respect to the field F and possess a multiplaction table

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n which the y's are numbers of F.
plex number whose coördinates x; are numbers of F. Then shall

Let x' = Ex,e; be another hypercom

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when ƒ is in F, so that multiplication is distributive. Under these assumptions, the set of all numbers (1) with coördinates in F shall be called a linear algebra over F.

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3. We assume that e, is a principal unit (modulus), so that ex = xe1 = x for every number x of the algebra, and write 1 for e1. We assume that every number of the algebra satisfies a quadratic equation with coefficients in F. If e2 + 2ae + b 0, (e + a)2 = a2-b, so that we may take the units to be 1, E2, En, where E Sii, a number of F. For i and j distinct and >1, E; ± E; satisfies a quadratic, so that (E; ± E;)2 = Sii + S;; ± (E¡E; + E;E;) is a linear function of E; ± E;. Thus E¡E; + E¡E¡ is a linear function of E; + E; and of E¡−E;, and hence is a number 2sji of F.

2sij

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Let u2,

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..., u, be arbitrary numbers of F and write U

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It is a standard theorem that Q can be reduced to Σc,v,2 by a linear transformation uk = Zak with coefficients in F and of determinant ‡0. Write

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Then 1, 2,

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k,l =2

(l = 2, . . ., n).

en are linearly independent and may be taken as the new

units of our algebra over F. Then

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