This post is a continuation of Positive operators II, We begin by recalling the main fact proved there, then explain how a classical binomial series leads to a functional calculus for the square root of a positive operator.
Corollary 1 Let
be a bounded self-adjoint positive operator on a pre-Hilbert space
. Then
(1) ![]()
This equality between the operator norm and the supremum of quadratic forms will be used repeatedly below, in particular to control powers of
and to justify convergence of operator series.
Binomial series
In this section we recall a classical binomial series expansion for
, discuss its convergence, and rewrite it in a form adapted to our later application to operators.
The philosophy is: first we understand the scalar series very well, then we simply replace the scalar variable by an operator and invoke a general result about Cauchy products in Banach algebras.
We want to “construct” a positive square root of a positive operator
in a way that mimics the construction of the square root of a positive number. Historians of mathematics tell us that the Babylonians already had an efficient algorithm for extracting square roots; it was later described by Heron of Alexandria. Here we deliberately use a different, and in practice terribly ineffective, method. What matters to us is existence, not computational efficiency: our method uses a Taylor (binomial) series expansion.
One cannot comfortably use the Taylor series of
at
, because the derivatives blow up there, but one can expand at
or, equivalently, consider the Taylor series of
at
.
Binomial series and its convergence
The series we need is discussed in many analysis textbooks, for instance in [1].
We have
(2) 
(3) 
(4) ![]()
with the convention that
.
It is known (see \cite[pp.\ 56–57]{knapp}) that the series in \eqref{eq1mx0} is uniformly convergent for
.
Notice that all
, and setting
we obtain
(5) 
Thus, at the scalar level, the coefficients
form a probability distribution on
(if one wishes to think probabilistically), and the corresponding power series converges uniformly on
.
Square Root Lemma
We now state the main result we want to prove in this post, and then explain how the binomial series and the Cauchy product theorem in Banach algebras yield the desired square root of a positive operator.
Theorem 1. [Square Root Lemma]
Let
be a bounded self-adjoint positive operator on a real or complex Hilbert space
.
Then there is a unique bounded positive self-adjoint operator
such that
.
Furthermore,
commutes with every bounded operator (linear or, if
is complex, also antilinear) which commutes with
.
Remark 1. In the proof below I essentially follow the method used in [2, Ch.\ VI.4, pp. 195–196]. As we shall see, this method works equally well for real Hilbert spaces.
Before we start the proof, let us make a couple of simple observations.
Let
be such that
. Then, for every integer
, we have
. Indeed, if
is even, then
![]()
and if
is odd, then
![]()
Suppose, additionally, that
. Then also
for all
. Indeed, from the corollary above we have, for
,
, and
, since again
.
Proof. We first prove existence.
Reduction to the case 
The case
is trivial, so we assume
. It is enough to consider the case
, or equivalently, since
,
. Indeed, in the general case we will define
![Rendered by QuickLaTeX.com \[ \sqrt{A}=\|A\|^{1/2}\,\sqrt{\frac{A}{\|A\|}}, \]](https://arkadiusz-jadczyk.eu/blog/wp-content/ql-cache/quicklatex.com-3a867caaf4428ac41f490c6b35031bd6_l3.png)
so the core of the argument is the construction for operators with spectrum contained in
.
So let us assume
.
Defining
via the binomial series
In the scalar formula \eqref{eq1mx} we replace the number
by the identity operator
and the scalar variable
by the operator
. Formally this gives
(6) 
We first verify that the series on the right-hand side of \eqref{eqsqrA} is absolutely convergent in
to a bounded self-adjoint operator. Indeed, since
, we have
![]()
which entails
![Rendered by QuickLaTeX.com \[ 1+\sum_{n=1}^{\infty} \|c_n A^n\| \leq 1+\sum_{n=1}^{\infty} c_n =2, \]](https://arkadiusz-jadczyk.eu/blog/wp-content/ql-cache/quicklatex.com-054034d1d767ba63020ed45a4d2eef9d_l3.png)
where we have used the fact that
and \eqref{eqcn1}.
Thus the series in \eqref{eqsqrA} converges absolutely in the Banach algebra
, and we can safely define
(7) 
The operator
is clearly self-adjoint, since each
is self-adjoint and the coefficients
are real.
Showing that 
How do we know that
is indeed equal to
, given that we are now dealing with a series of operators rather than numbers, as in \eqref{eq1mx}?
The key point is the Cauchy product formula for absolutely convergent series in a Banach algebra, proved in the Appendix below.
In the scalar case we know that \eqref{eq1mx} holds for all
. Taking the square of the series we formally compute
![Rendered by QuickLaTeX.com \[ \begin{split} \left(1-\frac12 x-\frac{1}{8}x^2+\cdots\right) \left(1-\frac12 x-\frac{1}{8}x^2+\cdots\right)\\ = 1-\frac12 x-\frac12 x-\frac{1}{8}x^2-\frac{1}{8}x^2+\frac{1}{4}x^2+\cdots\\ =1-x+0\cdot x^2+\cdots. \end{split} \]](https://arkadiusz-jadczyk.eu/blog/wp-content/ql-cache/quicklatex.com-d3aa7ddc6b855ccd79b2d52d059b9a00_l3.png)
Already the first two terms give the desired result
, so the coefficients in front of all powers
with
must cancel to zero. These coefficients are exactly those that appear when we form the Cauchy product of the series
![Rendered by QuickLaTeX.com \[ 1-\sum_{n=1}^{\infty}c_n x^n \]](https://arkadiusz-jadczyk.eu/blog/wp-content/ql-cache/quicklatex.com-e922a1ba2d84ff21dac30ca21c5473dd_l3.png)
with itself.
By the Cauchy product theorem in Banach algebras (see the Appendix), the same identities hold when we replace the scalar variable
by an operator
with
, provided the series is absolutely convergent. Therefore, for our operator series,
![Rendered by QuickLaTeX.com \[ B^2 = (I-\sum_{n=1}^{\infty}c_n A^n)^2 = I-A. \]](https://arkadiusz-jadczyk.eu/blog/wp-content/ql-cache/quicklatex.com-54e54ee9e5867cfdd888b4e2e883c083_l3.png)
This shows that
is indeed a square root of
.
Positivity of 
We must now show that
. To this end we notice that the coefficients in front of
, for
, are all negative. Taking into account the fact that
for all
, we obtain
(8) 
Hence
is self-adjoint and positive.
From
to 
We now replace, in Eq.\ \eqref{eqsqrA1}, the operator
by
, and thus
by
.
Notice that
is self-adjoint if and only if
is self-adjoint, and that
if and only if
. We obtain
(9) 
This
is again self-adjoint and positive, and satisfies
when
, hence in general, by the scaling reduction described earlier
(10) 
Commutation property
We now consider the \emph{commutation property} announced in the theorem.
It follows immediately from the construction above. The series in \eqref{eqsqrA2} is absolutely convergent. Therefore any bounded linear operator
(or, if
is complex, since the coefficients of the series are all real, also any bounded antilinear operator) that commutes with
commutes also with all partial sums of the series, and therefore, by continuity of the operator product, also with
defined in \eqref{eqsqrA2}. Thus
whenever
.
Uniqueness
Finally we show \emph{uniqueness}. Let
be defined as in Eq.\ \eqref{eqsqrA2}, and assume that
is another bounded self-adjoint positive operator with
.
First we show that
commutes with
. We have
, so
commutes with
. We already know that
commutes with every bounded operator commuting with
. Therefore
commutes with
.
Consider now the two operators
![]()
Since
are self-adjoint positive, and
is self-adjoint, both
and
are self-adjoint and positive. Moreover, using the commutativity of
and
, one sees that
![]()
We compute their sum:
![Rendered by QuickLaTeX.com \[ \begin{split} (B-B')B(B-B') + (B-B')B'(B-B')=\\ 2A(B-B')+2A(B'-B)=0. \end{split}\]](https://arkadiusz-jadczyk.eu/blog/wp-content/ql-cache/quicklatex.com-97f4485353be6d1ee61123e101afca2d_l3.png)
Since
and
, we get
![]()
and a short algebraic computation shows that
![]()
Thus
.
But
and
are self-adjoint positive, so their sum being zero implies that each of them must be zero separately, therefore their difference, which is
is also zero. If
, then also
. But ![]()
It follows that
.
This completes the proof of the theorem.
Corollary 2. Let
be two commuting bounded positive self-adjoint operators on
. Then their product
is self-adjoint positive.
Proof.
is evidently self-adjoint. We have
Since
is self-adjoint and
is positive,
is also positive.
Appendix: Cauchy Product of Absolutely Convergent Series in
a Banach Algebra
For completeness, and to make the “scalar-to-operator” transition completely transparent, we include here a standard result on Cauchy products in Banach algebras.
The proof is formally identical to the classical scalar case once
is replaced by the norm
and one uses completeness and continuity of multiplication.
Theorem. Let
be a Banach algebra over
, where
is
or
.
Let
and
be sequences in
such that the series
![Rendered by QuickLaTeX.com \[ \sum_{n=0}^{\infty} a_n \qquad\text{and}\qquad \sum_{n=0}^{\infty} b_n \]](https://arkadiusz-jadczyk.eu/blog/wp-content/ql-cache/quicklatex.com-4190a05be974636dab38a9d267653c0c_l3.png)
are absolutely convergent, i.e.
![Rendered by QuickLaTeX.com \[ \sum_{n=0}^{\infty} \|a_n\| < \infty, \qquad \sum_{n=0}^{\infty} \|b_n\| < \infty. \]](https://arkadiusz-jadczyk.eu/blog/wp-content/ql-cache/quicklatex.com-708dad7b5027deaf973dd171699c3126_l3.png)
Define the Cauchy product
by
![Rendered by QuickLaTeX.com \[ c_n := \sum_{k=0}^{n} a_k b_{n-k}, \qquad n \ge 0. \]](https://arkadiusz-jadczyk.eu/blog/wp-content/ql-cache/quicklatex.com-1768ba55555fd907edbbc087b8cf5903_l3.png)
Then the series
is absolutely convergent in
, and
![Rendered by QuickLaTeX.com \[ \sum_{n=0}^{\infty} c_n = \left(\sum_{n=0}^{\infty} a_n\right) \left(\sum_{n=0}^{\infty} b_n\right) \]](https://arkadiusz-jadczyk.eu/blog/wp-content/ql-cache/quicklatex.com-f00117ea314094735264f3618eab0c54_l3.png)
with multiplication in
.
Proof. Let
![Rendered by QuickLaTeX.com \[ A_N := \sum_{n=0}^{N} a_n,\qquad B_N := \sum_{n=0}^{N} b_n,\qquad C_N := \sum_{n=0}^{N} c_n \]](https://arkadiusz-jadczyk.eu/blog/wp-content/ql-cache/quicklatex.com-c49f37345f43aeb6f249aa6efad37599_l3.png)
denote the partial sums.
By completeness of
and absolute convergence, there exist
such that
![]()
as
.
We proceed in two steps.
Step 1: Absolute convergence of
.
For each
we have
![Rendered by QuickLaTeX.com \[ \|c_n\| = \left\| \sum_{k=0}^{n} a_k b_{n-k} \right\| \le \sum_{k=0}^{n} \|a_k b_{n-k}\| \le \sum_{k=0}^{n} \|a_k\|\,\|b_{n-k}\|, \]](https://arkadiusz-jadczyk.eu/blog/wp-content/ql-cache/quicklatex.com-dcf7c9e2c3f40651e10bc203bac8d351_l3.png)
using the triangle inequality and submultiplicativity of the norm.
Hence for each
,
![Rendered by QuickLaTeX.com \[ \sum_{n=0}^{N} \|c_n\| \le \sum_{n=0}^{N} \sum_{k=0}^{n} \|a_k\|\,\|b_{n-k}\| = \sum_{k+\ell \le N} \|a_k\|\,\|b_{\ell}\|, \]](https://arkadiusz-jadczyk.eu/blog/wp-content/ql-cache/quicklatex.com-422fe61363ff8a2c2ed603313090f33d_l3.png)
where we have reindexed by
.
Since
and
, we obtain the uniform bound
![Rendered by QuickLaTeX.com \[ \sum_{n=0}^{N} \|c_n\| \le \left(\sum_{k=0}^{\infty}\|a_k\|\right) \left(\sum_{\ell=0}^{\infty}\|b_{\ell}\|\right) < \infty \qquad \text{for all } N. \]](https://arkadiusz-jadczyk.eu/blog/wp-content/ql-cache/quicklatex.com-58f178e5897b35b987870261bd38e496_l3.png)
Thus the sequence of partial sums
is increasing and bounded,
hence convergent in
. This is exactly absolute convergence of
in
.
Step 2: Identification of the sum.
We first observe the combinatorial identity
(11) 
where
![Rendered by QuickLaTeX.com \[ d_{n}^{(N)} := \sum_{\substack{0 \le k,\ell \le N \\ k+\ell = n}} a_k b_{\ell}. \]](https://arkadiusz-jadczyk.eu/blog/wp-content/ql-cache/quicklatex.com-4f67202c4101405a708ca39e23f00b13_l3.png)
On the other hand, by definition of
we have
![Rendered by QuickLaTeX.com \[ c_n = \sum_{k=0}^{n} a_k b_{n-k}, \]](https://arkadiusz-jadczyk.eu/blog/wp-content/ql-cache/quicklatex.com-c2b493dcbbceb29542f10bf7f5ff5689_l3.png)
where the sum is finite for every
. Thus the family
is absolutely summable, and the finite sums in \eqref{eq:finite-cauchy} can be reorganized in terms of the
and “tail” terms.
More precisely, for each
we can write
![Rendered by QuickLaTeX.com \[ A_N B_N = \sum_{n=0}^{N} c_n + R_N, \]](https://arkadiusz-jadczyk.eu/blog/wp-content/ql-cache/quicklatex.com-4e2dd786c564e644f0239fa55ea2b938_l3.png)
where
is the sum of all terms
with
and
.
Equivalently,
![]()
We claim that
as
. Indeed, by the triangle inequality and submultiplicativity,
![Rendered by QuickLaTeX.com \[ \|R_N\| \le \sum_{\substack{0 \le k,\ell \le N \\ k+\ell > N}} \|a_k\|\,\|b_{\ell}\|. \]](https://arkadiusz-jadczyk.eu/blog/wp-content/ql-cache/quicklatex.com-bf6590cb8677b3b17b986a9b77212a11_l3.png)
Let
be given.
By absolute convergence, choose
such that
![]()
Then, for all
, any pair
with
and
must satisfy at least one of
or
.
Hence
![Rendered by QuickLaTeX.com \[ \|R_N\| \le \sum_{\substack{0 \le k,\ell \le N \\ k+\ell > N}} \|a_k\|\,\|b_{\ell}\| \le \sum_{k\ge K} \|a_k\| \sum_{\ell\ge 0} \|b_{\ell}\| + \sum_{\ell\ge K} \|b_{\ell}\| \sum_{k\ge 0} \|a_k\|. \]](https://arkadiusz-jadczyk.eu/blog/wp-content/ql-cache/quicklatex.com-919bb7f2546bacbdddb680cacf9cfdb0_l3.png)
The right-hand side is bounded by
![Rendered by QuickLaTeX.com \[ \varepsilon \sum_{\ell\ge 0} \|b_{\ell}\| + \varepsilon \sum_{k\ge 0} \|a_k\| = \varepsilon \left( \sum_{\ell\ge 0} \|b_{\ell}\| + \sum_{k\ge 0} \|a_k\| \right), \]](https://arkadiusz-jadczyk.eu/blog/wp-content/ql-cache/quicklatex.com-4709fbe7d79143e2c6486a2d26cabc4f_l3.png)
which is independent of
. Thus
can be made arbitrarily small by choosing
(and then
)
sufficiently large; in particular,
![]()
Since
and
, and multiplication is continuous in the
Banach algebra
, we have
as
. Using
and
, we obtain
![]()
But the limit of
is by definition the sum of the absolutely convergent series
.
This proves that
![Rendered by QuickLaTeX.com \[ \sum_{n=0}^{\infty} c_n = AB = \left(\sum_{n=0}^{\infty} a_n\right) \left(\sum_{n=0}^{\infty} b_n\right), \]](https://arkadiusz-jadczyk.eu/blog/wp-content/ql-cache/quicklatex.com-dddd7393b87344c6634d001a29b252be_l3.png)
as claimed.
Remark The proof is formally identical to the classical scalar case once
is replaced by the norm
and one uses completeness
and continuity of multiplication in the Banach algebra.
Afternotes.
20-06-26 Added Corollary 2.
References.
\[1] Knapp, A.~W., Basic Real Analysis. Digital Second Edition.
[2] Reed, M., Simon, B., Methods of Modern Mathematical Physics, I: Functional Analysis, Academic Press, 1980.