Abstract
Given an arbitrary state \(\rho \) and some figure of merit \(\mathcal{E}(\rho )\), it is usually a hard problem to determine the value of \(\mathcal{E}(\rho ^{\otimes N})\). One noticeable exception is the case of additive measures, for which we simply have \(\mathcal{E}(\rho ^{\otimes N}) = Ne\), with \(e\equiv \mathcal{E}(\rho )\). In this work, we study measures that can be described by \(\mathcal{E}(\rho ^{\otimes N}) =E(e;N) \ne Ne\), that is, measures for which the amount of resources of N copies is still determined by the single real variable e, but in a nonlinear way. If, in addition, the measures are analytic around \(e=0\), recurrence relations can be found for the Maclaurin coefficients of E for larger N. As an example, we show that the \(\ell _1\)-norm of coherence is a non-trivial case of such a behavior.


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The term “resource” is employed in the general sense, since the results to be derived do not rely on all the requirements for a quantity to be a resource (in the resource-theoretic sense).
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Acknowledgements
The authors thank Bárbara Amaral and Nadja Bernardes for a discussion on the topics addressed in this manuscript. This work received financial support from the Brazilian agencies Coordenação de Aperfeiçoamento de Pessoal de Nível Superior (CAPES), Fundação de Amparo à Ciência e Tecnologia do Estado de Pernambuco (FACEPE), and Conselho Nacional de Desenvolvimento Científico e Tecnológico through its program CNPq INCT-IQ (Grant 465469/2014-0).
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Appendices
Third-order coefficient solution
To solve the recurrence relation (8), we choose \(K=a\) and apply the known solutions for \(d_1(a^n)\) and \(d_2(a^n)\) [8]:
Remember that \(a^n=N\). The recursive substitution of \(d_3(a^{n})\) into itself \(l=n-1\) times gives:
Redefining all sums to start at \(l=0\) and using the geometric series \(\sum _{l=0}^{n-1}x^l=\frac{1-x^{n}}{1-x}\), we get the third order in (9):
Binomial coefficients
We start with (4) for \(K=2\) (here the index l is rewritten as \(j-k\)):
Remember that \(N \in \mathbb {P}_{2}\), so \(\frac{N}{2}\) is an integer. The hypothesis that only \(d_1(2)\) and \(d_2(2)\) are nonzero means that \(\pi _i(j,l;2)\) is a product of combinations of these two quantities only, so we need to consider the composition of j using only the numbers 1 and 2, which has \(\tiny {\frac{(j-k)!}{k!(j-2k)!}}\) elements, for k repetitions of the number 2 (the maximum value of k is \(\lfloor \frac{j}{2} \rfloor \)), so:
Putting (21) into (20) and considering the case \(E^{(a=2)}(e)=2e+d_2(2)e^2\), we find the following recurrence relation:
Now we test expression \(d_j(N)=[d_2(2)]^{j-1}\tiny {{{N} \atopwithdelims (){j}}}\), induced in (11). Using the subset-of-a-subset property [22], we get:
For the evaluation of the sum in (22), we take the integral representation \(\tiny {\left( \begin{array}{c} n \\ m \end{array} \right) } = \frac{1}{2\pi i} \oint _{\Gamma } \frac{(1+z)^n}{z^{m+1}} dz\) to solve the problem using the Egorychev method [23, 24], where z is a complex variable and \(\Gamma \) is a small closed contour around \(z=0\):
Is easy to see that for \(\lfloor \frac{j}{2} \rfloor<k<\frac{N}{2}\) the integral vanishes. By making \(k=\lfloor \frac{j}{2} \rfloor +l\) (so \(l \le \frac{N}{2}- \lfloor \frac{j}{2} \rfloor \)), the integrand does not have residue at \(z=0\) for any value of \(l \in (1,\frac{N}{2}- \lfloor \frac{j}{2} \rfloor )\) and, therefore, we can rewrite the sum with upper limit equal to \(\frac{N}{2}\). Then, we can use the binomial theorem:
After some cancellations, we make a simple change of variables \(z\,\rightarrow \,2z'\) (\(\Gamma \rightarrow \Gamma '\)) and the integral becomes exactly the Cauchy integral representation of the binomial coefficient, so the proposition is proven.
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Melo, L.F., Parisio, F. Simplest non-additive measures of quantum resources. Quantum Inf Process 20, 355 (2021). https://doi.org/10.1007/s11128-021-03297-5
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DOI: https://doi.org/10.1007/s11128-021-03297-5