Abstract
Two generalizations U( + )y() = U()y( + ) (, , A) of the functional equation of the mean sun are studied, where (A, +) is an Abelian group, K is a field, n is a positive integer, and both y: A Kn and U: A GL(n, k) (or U: A Mn(k) in the second case) are unknown functions, which will be determined by the equation. |
Local solar time is measured by a sundial. When the center of the sun is on an observer’s meridian, the observer’s local solar time is zero hours (noon). Because the earth moves with varying speed in its orbit at different times of the year and because the plane of the earth’s equator is inclined to its orbital plane, the length of the solar day is different depending on the time of year. It is more convenient to define time in terms of the average of local solar time. Such time, called mean solar time, may be thought of as being measured relative to an imaginary sun (the mean sun) that lies in the earth’s equatorial plane and about which the earth orbits with constant speed. Every mean solar day is of the same length.1
In [1, 4] it is shown that the mean sun satisfies the functional equation
| (1) |
Then M(, )y(s) is the direction from the earth to the sun expressed in a local coordinate system on the surface of the earth in the point of longitude and latitude .
In the present paper we investigate generalizations of equation (1) for fixed . To be more precise, first we will solve the following functional equation
| (2) |
We will mainly deal with problems of the second and third kind.
In Theorem 6 we describe in an appropriate system of coordinates the structure of the space SU of all solutions of (2) for a given U: A GL(n, K). We also state in this theorem how such a mapping U necessarily looks if a nontrivial solution y (i.e. y0) exists. A similar description of U-invariant subspaces of SU is given in Theorem 8. We emphasize that by our result (and similarly by the following theorems) the problem of solving (2) can be reduced, at least to some extent, to the problem of finding all exponential functions U11: A GL(k, K) (cf. the representation of U in Theorem 6), i.e. non singular matrices U11() satisfying the equation
Here we assume that these functions are known and we refer the reader to [3].
In Theorem 9 we construct to a given subspace S0 of Kn the set of all mappings U and correspondingly the space S of all functions y, such that (U, y) satisfies (2) and S0 is exactly the set of all initial values y(0) for y S. It is clear that this yields together with Theorem 6 an implicit description of the set of all solutions (U, y) of (2) by varying the subspace S0 of Kn. However, the space S and the mapping U obtained in this way from S0 may have the property that S is a proper subset of SU . Therefore we also deal with the problem to characterize the situation when S = SU .
From a mathematical point of view it seems also interesting to study the functional equation (2) for mappings U: A Mn(K). This situation is more complicated both with respect to the technical details and the construction (description) of the solutions U or y or (U, y). In Theorem 20 we start from a given mapping U: A Mn(K) and describe completely in appropriate coordinates the set of all functions y: A Kn, such that (U, y) is a solution of (2). Again this theorem provides necessary conditions on U for the existence of nontrivial solutions y of (2). We also show in Theorem 21 how to construct all mappings U: A Mn(K) and corresponding spaces S of functions y: A Kn, such that is a given subspace S0 of Kn and (U, y) is a solution of (2), hence giving an implicit description of the general solution of (2) by varying S0. However, we were not able to contribute to the problem when S = SU .
The main difficulties in this last part seem to arise from the fact that there can occur solutions y (to a given U) with y(0) = 0 but y0 (cf. Lemma 18).
Here in this part we always assume that U is a mapping from the abelian group A to GL(n, K).
Lemma 1. Let B, C be matrices in GL(n, k). Then (U, y) is a solution of (2) if and only if (V, By) is a solution of (2), where V () = CU()B-1.
For C = U(0)-1 we get CU(0) = I n, the identity matrix. Hence, without loss of generality we will always assume that U(0) = In.
It is also possible to reverse the statement of Lemma 2.
Lemma 3. Assume U(0) = In and let y be given by (3). If (U, y) satisfies (4), then (U, y) is a solution of (2).
For any mapping U: A GL(n, k) let
Some basic properties of these two sets are collected in the following
Lemma 4. Both SU and SU0 are K-linear spaces and : SU0 SU , given by (y0) := U(.)y0, is a vector space isomorphism.
In conclusion, both SU and SU0 are m-dimensional linear spaces for some 0 < m < n.
There are some more interesting properties of SU and SU0.
If denotes a basis of SU0, then there exists a matrix B GL(n, k), such that Bbi = ei, the i-th unit vector in Kn. Applying this matrix B as a coordinate transformation on Kn as in Lemma 1 we get that SUB-1 - 1 = <e 1, ..., em>, the m-dimensional linear space generated by the first m unit vectors in Kn. Thus without loss of generality we may assume that SU = <e1, ..., em>.
Theorem 6. Let U: A GL(n, K) be a mapping, such that SU0 = <e1, ..., em> and U(0) = In. Then U() can be partitioned as a block matrix of the form
where U11() GL(m, K), U22() GL(n - m, K) and U12() Mm,n-m(K). These matrices satisfy the boundary conditions U11(0) = Im, U22(0) = In-m and U12(0) = (0)m,n-m, the zero matrix. Moreover, U11 is an exponential function, i.e. U11( + ) = U11()U11() for all , A.
Each y SU can be expressed as
and (0) Km.
| (5) |
which means that U11( + ) (0) = U11()U11() (0) for all (0) Km and , A, so that U11 is an exponential function.
We are also interested in subspaces of SU . First we present a generalization of Lemma 5.
Lemma 7. Let S be a subspace of SU . Then the following statements are equivalent:
To each y0 S0 there exists y S, such that y0 = y(0). Under the assumption 2, the function z() := y( + 0) belongs to S for any 0 A. So z(0) S0 and z(0) = y(0) = U(0)y(0) = U(0)y0 by (3). Thus we proved that 2 implies 3.
In order to close the cycle of implications take y S. Then y(0) S0. For arbitrary 0 A also U(0)y(0) belongs to S0. Hence, there exists z S such that z(0) = U(0)y(0). Taking into account that S is a subspace of SU we can write z as z() = U()z(0) = U()U(0)y(0) = U( + 0)y(0) = U(0)U()y(0) = U(0)y() by (3), (4), (4) and (3). Thus U(0)y S.
A generalization of Theorem 6 is
Theorem 8. Let S be a k-dimensional U-invariant subspace of SU . Then there exist coordinates in Kn, such that S0 = <e 1, ..., ek>, and U() is a block matrix of the form
| (6) |
for Kk.
So far we described solutions (U, y) of (2) when the mapping U was given. Now we will assume that a linear subspace S0 of Kn is given and we describe all solutions (U, y) of (2), such that SU0 = S0. Let S0 be a k-dimensional U-invariant subspace of Kn, then without loss of generality S0 = <e 1, ..., ek>.
Theorem 9. Let S0 = <e 1, ..., ek> be a subspace of Kn, and let U 11() GL(k, K), U22() GL(n - k, K) and U12() Mk,n-k(K), such that U11(0) = Ik, U22(0) = In-k, U12(0) = (0)k,n-k. Moreover U11 is assumed to be an exponential function. Then
is a U-invariant subspace of SU , where U is given by (6).
When does S = SU hold?
Lemma 10. The two spaces S and SU coincide if and only if for all Kn-k \ there exists (0, 0) A2, such that
| (7) |
which finishes the proof.
Now we are going to present several examples for the situation S = SU , i.e. by Lemma 10 examples, where condition (7) is satisfied. Here we always assume that A = K. First we will deal with the second line of condition (7). Secondly, if this condition is not satisfied by all , then let V denote the set
Thus V is an r-dimensional subspace of Kn-k for 0 < r < n - k. In order to satisfy the requirements of Lemma 10 in this situation as well, the first line in (7) must be satisfied for V .
Now we describe some examples how to construct U22: K GL(s, K) for s < n - k, such that
| (8) |
Now we describe examples how to construct U12: K Mk,n-k(K), such that
| (9) |
where the upper part is -Ir and the lower part is a 0-matrix of the dimension (k - r) × r. Then for 0 = 0 = 1 we get that U11(1)U12(1) + U12(1)U22(1) - U12(1 + 1) = -U12(2) and it is obvious that -U12(2)0 for all Kr \ .
For k < r one possible way to proceed is indicated in
Lemma 11. If there are enough elements in K, to be more precise, if > 2 + 1, then it is always possible to find 0 and 0 satisfying (9).
If q > 1 and is big enough, then there exists 2 K \ and we assume that
Going on like this we can find elements 1, ..., q K and matrices U12(±i). If s > 0 and is big enough, then there exists q+1 K \ and we assume that
When Kr \ , then there exists 1 < i < r, such that i0. Hence, there exists j , such that (j - 1)k < i < jk. For 0 = j and 0 = -j we have U11(j)U12(-j) + U12(j)U22(-j) - U12(0) = 2U12(j)U22(-j). According to the choice of i and j it is clear that (9) is satisfied.
This is a very general result, but it is not the best result which is possible.
then for 0 = 1 and 0 = we get U11(1)U12() + U12(1)U22() - U12( + 1) = U12( + 1) and (9) is satisfied. For k < r the following lemma holds:
Lemma 13. If there are enough elements in K, to be more precise, if > 2 + 2, then it is always possible to find 0 and 0 satisfying (9).
If s > 0 and is big enough, then there exists q+1 K, such that q+1, q+1 + 1 K \ and we assume that
Given Kr \ there exists 1 < i < r, such that i0. Hence, there exists j , such that (j - 1)k < i < jk. For 0 = j and 0 = 1 we have U11(j)U12(1) + U12(j)U22(1) - U12(j + 1) = -U12(j + 1). According to the choice of i and j it is clear that (9) is satisfied.
then (9) is satisfied. For r = 2 assume that U11(1) is given as above and
then again (9) is satisfied. For k = r = 3 and for any choice of U11(1), U22(1) GL(3, K) of order dividing 2 the computer did not find a matrix U12(1) in M3(K) such that (9) is satisfied. Other cases were not studied so far.
If k > r it is not possible to satisfy (9), since there is only one possible choice 0 = 0 = 1, which determines exactly one matrix U11(1)U12(1) + U12(1)U22(1). This matrix describes a homomorphism from Kk to Kr, which has a kernel of dimension > k - r > 0.
In this part we generalize the functional equation (2) by assuming that U() is not necessarily a regular matrix, i.e. U: A Mn(K). Also in this situation Lemma 1 holds. When we define SU and SU0 as it was done earlier, then SU and SU0 are K-linear spaces (cf. Lemma 4). Again SU0 is an m-dimensional subspace of Kn for 0 < m < n, and S U is invariant under translations, and SU0 = (cf. Lemma 5). Without loss of generality we can assume (as in the earlier case) that there exists a basis of Kn, such that SU0 = <e1, ..., em>.
Since U(0) need not be a regular matrix, we do not get the results of Lemma 2, and in general there is no isomorphism between SU and SU0.
For = = 0 or = 0 we derive from (2)
If U() is partitioned as in (5) and y() is written as for () Km, then from (10) we get
which leads to the system of equations
| (12) |
Lemma 15. Let (U, y) be a solution of (2). Then there exists a system of coordinates of Kn, such that
| (13) |
| (14) |
and
Without loss of generality assume that U = V . From the second line of (12) we deduce that 0 = 0 () = U21() (0) for all A. Since (0) can arbitrarily be chosen in Km, it is clear that U21() = (0)n-m,m for all A.
Since SU0 = <e1, ..., em>, there exist y1, ..., ym SU , such that yj(0) = ej, the j-th unit vector in Kn, for 1 < j < m. Let S U ' := <y 1, ..., ym>, then SU ' is an m-dimensional subspace of SU . In order to prove this, it is only necessary to show that y1, ..., ym are linearly independent. Let 1, ..., m K, such that i = 1miyi = 0, then also i = 1miyi(0) = 0, which implies i = 1miei = 0, so that 1 = ... = m = 0.
For y SU ' there exist uniquely defined 1, ..., m K such that y = i = 1miyi. These i can be read from y(0), since y(0) = i = 1miei.
Define the m × m-matrix Y () corresponding to the chosen y1, ..., ym by
| (15) |
| (16) |
These equations are collected to the matrix equation
| (17) |
Again these equations can be collected for j = 1, ..., m and we derive
| (18) |
| (19) |
such that Y 11() is a k × k-matrix. We note that the “auxiliary” matrix function Y : A Mm(K), which will help us to describe the space SU of solutions y (for given U), is in general not uniquely determined. However, from (17), from the decomposition of U11(0) in Lemma 15 and the corresponding decomposition of Y () we see that Y 11() and Y 12() are uniquely determined by U11(), namely
| (20) |
and we end up with the system of equations
| (21) |
| (22) |
| (23) |
Then it is possible to find a matrix B'' GL(m - k, K), such that the coordinate transformation on Km induced by
satisfies
Let B be the corresponding coordinate transformation on Kn
If U is decomposed as in (13) and (14), then also UB has this property.
Without loss of generality we assume that the basis of Kn was chosen in such a way that Lemma 15 is satisfied and that and are a basis of V or W respectively. Then it is useful and important to partition Y () further as a 3 × 3 block matrix of the form
such that Z11() = Y 11() Mk(K), Z22() Mm-k-r(K) and Z33() Mr(K). Hence
Let x = denote a vector in Km-k, where Km-k-r and Kr. Then x belongs to W if and only if = 0. Moreover Y 12()|W = 0 for all A, which means Z13() = (0)k,r for all A. From the definition of W it is clear that Z12() = 0 for all A is equivalent to = 0.
The first line of (21) reads now as
From the second line of (21) we derive
and
Hence, each column of Z23() is 0 Km-k-r, so that Z 23() = (0)m-k-r,m-k-r for all A.
From (22) we deduce
Let M denote the matrix between the two braces [ and ], then each column of M is 0 Km-k-r and consequently M = (0) m-k-r,k. Hence, we proved that
The same way we deduce from (23) that
and correspondingly
This finishes the proof of
Theorem 16. There exists a coordinate system of Km, such that Y () is a solution of (19) if and only if Y () can be written as
where
is an exponential function, Z11() Mk(K), Z22() Mm-k-r(K), Z33() Mr(K), satisfying the conditions Z11(0) = Ik, Z22(0) = Im-k-r, Z33(0) = Ir, Z12(0) = (0)k,m-k-r, Z21(0) = (0)m-k-r,k, Z31(0) = (0)r,k and Z32(0) = (0)r,m-k-r. For 0 the matrices Z31(), Z32(), Z33() can be arbitrarily chosen.
Next we describe the structure of SU in more details.
Lemma 17. For each y SU with y(0)0 there exists a subspace SU ' of S U , such that y SU '.
Let N(SU ) denote the set . Then N(SU ) is a subspace of SU . The appearance of this subspace N(SU ) of SU , which is in general not , is one of the main differences to the case of mappings U: A GL(n, K). We will see that N(SU ) is closely related to the space W . This is described in
so that () = 0 for all A. For = 0 we derive
so that Y 12() () = 0 for all , A. This however implies that () W for all A.
Assuming conversely that (0) = 0, () = 0 and () W for all A, then it is obvious that z N(SU ).
In conclusion we get the following result:
Lemma 19. Let SU ' be an m-dimensional subspace of S U (constructed as above), then SU = SU ' N(S U ).
We notice that in the decomposition SU = SU ' N(S U ) the space SU ' is in general not uniquely determined, whereas N(SU ) is unique by definition. However, SU ' can be any m-dimensional subspace of SU , such that the space of initial values y(0) (for y SU ') is already SU0.
As an immediate consequence we get
The following Theorem 20 yields together with Theorem 16 the structure of the space SU , of all solutions of (2), for a given function U: A Mn(K). These theorems also contain necessary conditions on U in order to admit a nontrivial solution y.
Theorem 20. Let U: A Mn(K) be given and assume that dim SU0 = m. Then there exist coordinates in Kn and solutions (U, y j) of (2) for j = 1, ..., m, such that yj(0) = ej. Moreover, U() can be written as in (13) and U11() satisfies (20). Y 11() and Y 22() are the blocks in the first row of the matrix Y () given by (15). This matrix is also a solution of (19) and each element y of SU can be expressed as y() = for given by (16) with arbitrary (0) Km and () given by (24).
We finish by Theorem 21, which provides a construction of all solutions (U, y) of (2) by starting from an arbitrary subspace of initial values y(0) of Kn. This choice then leads via the block matrix Y () satisfying (19) to a matrix valued function U and a space S of solutions corresponding to U. In this general situation we do not discuss the problem when S = SU .
Theorem 21. If Y () satisfies (19), U11() is given by (20), is given by (16) for arbitrary (0) Km and () given by (24), then (U, y) is a solution of (2) for
We can rewrite U11(0)[Y ( + )Y () - Y ()Y ( + )] as U11(0)[Y ( + )Y () - Y ( + + ) + Y ( + + ) - Y ()Y ( + )] = U11(0)[Y ( + )Y () - Y ( + + )] + U11(0)[Y ( + + ) - Y ()Y ( + )], which is equal to (0)m,m since (19) holds.
In order to determine all solutions (U, y) of (2) we start with an arbitrary m-dimensional subspace S0 of Kn for some 0 < m < n. Let be a basis of S0, then there exists a matrix B GL(n, K), such that Bbi = ei for 1 < i < m. Hence BS0 = <e 1, ..., em>. For each solution Y () of (19) described in Theorem 16 let U11() be given by (20) and U() be given by (13) with arbitrary matrices U12() and U22(). Then each element y of
is together with U a solution of (2). Due to this construction T 0, the space of initial values y(0) for y T , is equal to <e1, ..., em>. According to Lemma 1 each pair (UB, B-1y) for y T is a solution of (2) and = S0. Hence, by varying S0 over all subspaces of Kn we determine all solutions (U, y) of (2).
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[4] J. Schwaiger. Some applications of functional equations in astronomy. Aequationes Mathematicae, 60 (2000), p. 185. In Report of the meeting, The Thirty-seventh International Symposium on Functional Equations, May 16-23, 1999, Huntington, WV.
HARALD FRIPERTINGER
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