Prof. Dr. Robert König



Teaching
 Funktionentheorie (SS 2016)
 Quantum Information Theory (SS 2016, with M. Wolf)
 Fallstudien der Mathematischen Modellbildung (WS 2015/2016)
 Reading group: Operator spaces (WS 2015/2016)
 Representations of compact groups (SS 2015)
 Entropie und Informationstheorie (SS 2015)
Research interests
 Quantum communication theory and cryptography
 Faulttolerant quantum information processing
 Topological quantum computation
 Manybody physics and variational methods
Publications
[Show/hide abstracts]
 M. E. Beverland, O. Buerschaper, R. König, F. Pastawski, J. Preskill and S. Sijher.
Protected gates for topological quantum field theories.
Journal of Mathematical Physics, 57, 022201, February 2016. arXivWe study restrictions on localitypreserving unitary logical gates for topological quantum codes in two spatial dimensions. A localitypreserving operation is one which maps local operators to local operators — for example, a constantdepth quantum circuit of geometrically local gates, or evolution for a constant time governed by a geometrically local boundedstrength Hamiltonian. Localitypreserving logical gates of topological codes are intrinsically fault tolerant because spatially localized errors remain localized, and hence sufficiently dilute errors remain correctable. By invoking general properties of twodimensional topological field theories, we find that the localitypreserving logical gates are severely limited for codes which admit nonabelian anyons, in particular, there are no localitypreserving logical gates on the torus or the sphere with M punctures if the braiding of anyons is computationally universal. Furthermore, for Ising anyons on the Mpunctured sphere, localitypreserving gates must be elements of the logical Pauli group. We derive these results by relating logical gates of a topological code to automorphisms of the Verlinde algebra of the corresponding anyon model, and by requiring the logical gates to be compatible with basis changes in the logical Hilbert space arising from local Fmoves and the mapping class group.
 R. König.
The conditional entropy power inequality for Gaussian quantum states.
Journal of Mathematical Physics, 55, 022201, February 2015. arXivWe propose a generalization of the quantum entropy power inequality involving conditional entropies. For the special case of Gaussian states, we give a proof based on perturbation theory for symplectic spectra. We discuss some implications for entanglementassisted classical communication over additive bosonic noise channels.
 R. König and J. Smolin.
How to efficiently select an arbitrary Clifford group element.
Journal of Mathematical Physics, 55, 122202, December 2014. arXivWe give an algorithm which produces a unique element of the Clifford group C_{n} on n qubits from an integer 0i <  C_{n} (the number of elements in the group). The algorithm involves O(n^{3}) operations. It is a variant of the subgroup algorithm by Diaconis and Shahshahani which is commonly applied to compact Lie groups. We provide an adaption for the symplectic group Sp(2n, F_{2}) which provides, in addition to a canonical mapping from the integers to group elements g, a factorization of g into a sequence of at most 4n symplectic transvections. The algorithm can be used to efficiently select randomelements of C_{n} which is often useful in quantum information theory and quantum computation. We also give an algorithm for the inverse map, indexing a group element in time O(n^{3}).
 R. König and F. Pastawski.
Generating topological order: no speedup by dissipation.
Physical Review B, 90, 045101, July 2014. arXivWe consider the problem of converting a product state to a ground state of a topologically ordered system through a locally generated opensystem dynamic. Employing quantuminformation tools, we show that such a conversion takes an amount of time proportional to the diameter of the system. Our result applies to typical twodimensional topologically ordered systems as well as, for example, the threedimensional and fourdimensional toric codes. It is tight for the toric code, giving a scaling with the linear system size. Our results have immediate operational implications for the preparation of topologically ordered states, a crucial ingredient for topological quantum computation: Dissipation cannot provide any significant speedup compared to unitary evolution.
 R. König and G. Smith.
The entropy power inequality for quantum systems.
IEEE Transactions on Information Theory, vol. 60, no. 3, pp. 15361548, March 2014. arXivWhen two independent analog signals, X and Y are added together giving Z = X + Y, the entropy of Z, H(Z), is not a simple function of the entropies H(X) and H(Y), but rather depends on the details of X and Y's distributions. Nevertheless, the entropy power inequality (EPI), which states that exp[2H(Z)] exp[2H(X)] + exp[2H(Y)], gives a very tight restriction on the entropy of Z. This inequality has found many applications in information theory and statistics. The quantum analogue of adding two random variables is the combination of two independent bosonic modes at a beam splitter. The purpose of this work is to give a detailed outline of the proof of two separate generalizations of the entropy power inequality to the quantum regime. Our proofs are similar in spirit to standard classical proofs of the EPI, but some new quantities and ideas are needed in the quantum setting. Specifically, we find a new quantum de Bruijin identity relating entropy production under diffusion to a divergencebased quantum Fisher information. Furthermore, this Fisher information exhibits certain convexity properties in the context of beam splitters.
 J. Dengis, R. König and F. Pastawski.
An optimal dissipative encoder for the toric code.
New Journal of Physics, 16, 013023, October 2013. arXivWe consider the problem of preparing specific encoded resource states for the toric code by local, timeindependent interactions with a memoryless environment. We propose a construction of such a dissipative encoder which converts product states to topologically ordered ones while preserving logical information. The corresponding Liouvillian is made up of fourlocal Lindblad operators. For a qubit lattice of size L x L, we show that this process prepares encoded states in time O(L), which is optimal. This scaling compares favorably with known local unitary encoders for the toric code which take time of order (L^{2}) and require active timedependent control.
 R. König and S. Bravyi.
Classification of topologically protected gates for local stabilizer codes.
Physical Review Letters, vol. 110, no. 170503, April 2013. arXivGiven a quantum error correcting code, an important task is to find encoded operations that can be implemented efficiently and faulttolerantly. In this Letter we focus on topological stabilizer codes and encoded unitary gates that can be implemented by a constantdepth quantum circuit. Such gates have a certain degree of protection since propagation of errors in a constantdepth circuit is limited by a constant size light cone. For the 2D geometry we show that constantdepth circuits can only implement a finite group of encoded gates known as the Clifford group. This implies that topological protection must be "turned off" for at least some steps in the computation in order to achieve universality. For the 3D geometry we show that an encoded gate U is implementable by a constantdepth circuit only if the image of any Pauli operator under conjugation by U belongs to the Clifford group. This class of gates includes some nonClifford gates such as the /8 rotation. Our classification applies to any stabilizer code with geometrically local stabilizers and sufficiently large code distance.
 R. König and G. Smith.
The classical capacity of quantum thermal noise channels to within 1.45 bits.
Physical Review Letters, vol. 110, no. 040501, January 2013. arXivWe find a tight upper bound for the classical capacity of quantum thermal noise channels that is within 1/ln 2 bits of Holevo's lower bound. This lower bound is achievable using unentangled, classical signal states, namely displaced coherent states. Thus, we find that while quantum tricks might offer benefits, when it comes to classical communication they can only help a bit.
 R. König and G. Smith.
Limits on classical communication from quantum entropy power inequalities.
Nature Photonics, vol. 7, pp. 140146, January 2012. arXivAlmost all modern communication systems rely on electromagnetic fields as a means of information transmission, and finding the capacities of these systems is a problem of significant practical importance. The Additive White Gaussian Noise (AWGN) channel is often a good approximate description of such systems, and its capacity is given by a simple formula. However, when quantum effects are important, estimating the capacity becomes difficult: a lower bound is known, but a similar upper bound is missing. We present strong new upper bounds for the classical capacity of quantum additive noise channels, including quantum analogues of the AWGN channel. Our main technical tool is a quantum entropy power inequality that controls the entropy production as two quantum signals combine at a beam splitter. Its proof involves a new connection between entropy production rates and a quantum Fisher information, and uses a quantum diffusion that smooths arbitrary states towards gaussians.
 S. Bravyi and R. König.
Classical simulation of dissipative fermionic linear optics.
Quantum Information and Computation, vol. 12, pp. 925943, November 2012. arXivFermionic linear optics is a limited form of quantum computation which is known to be efficiently simulable on a classical computer. We revisit and extend this result by enlarging the set of available computational gates: in addition to unitaries and measurements, we allow dissipative evolution governed by a Markovian master equation with linear Lindblad operators. We show that this more general form of fermionic computation is also simulable efficiently by classical means. Given a system of N fermionic modes, our algorithm simulates any such gate in time O(N^{3}) while a singlemode measurement is simulated in time O(N^{2}). The steady state of the Lindblad equation can be computed in time O(N^{3}).
 S. Bravyi and R. König.
Disorderassisted error correction in Majorana chains.
Communications in Mathematical Physics, vol. 361, pp. 641692, October 2012. arXivIt was recently realized that quenched disorder may enhance the reliability of topological qubits by reducing the mobility of anyons at zero temperature. Here we compute storage times with and without disorder for quantum chains with unpaired Majorana fermions  the simplest toy model of a quantum memory. Disorder takes the form of a random sitedependent chemical potential. The corresponding oneparticle problem is a onedimensional Anderson model with disorder in the hopping amplitudes. We focus on the zerotemperature storage of a qubit encoded in the ground state of the Majorana chain. Storage and retrieval are modeled by a unitary evolution under the memory Hamiltonian with an unknown weak perturbation followed by an errorcorrection step. Assuming dynamical localization of the oneparticle problem, we show that the storage time grows exponentially with the system size. We give supporting evidence for the required localization property by estimating Lyapunov exponents of the oneparticle eigenfunctions. We also simulate the storage process for chains with a few hundred sites. Our numerical results indicate that in the absence of disorder, the storage time grows only as a logarithm of the system size. We provide numerical evidence for the beneficial effect of disorder on storage times and show that suitably chosen pseudorandom potentials can outperform random ones.
 R. König, S. Wehner and J. Wullschleger.
Unconditional security from noisy quantum storage.
IEEE Transactions on Information Theory, vol. 58, no. 3, pp. 1962 1984, March 2012. arXivWe consider the implementation of twoparty cryptographic primitives based on the sole assumption that no largescale reliable quantum storage is available to the cheating party. We construct novel protocols for oblivious transfer and bit commitment, and prove that realistic noise levels provide security even against the most general attack. Such unconditional results were previously only known in the socalled boundedstorage model which is a special case of our setting. Our protocols can be implemented with presentday hardware used for quantum key distribution. In particular, no quantum storage is required for the honest parties.
 S. Beigi and R. König.
Simplified instantaneous nonlocal quantum computation with applications to positionbased cryptography.
New Journal of Physics, vol. 13, 093036, September 2011. arXivInstantaneous measurements of nonlocal observables between spacelike separated regions can be performed without violating causality. This feat relies on the use of entanglement. Here we propose novel protocols for this task and the related problem of multipartite quantum computation with local operations and a single round of classical communication. Compared to previously known techniques, our protocols reduce the entanglement consumption by an exponential amount. We also prove a linear lower bound on the amount of entanglement required for the implementation of a certain nonlocal measurement. These results relate to positionbased cryptography: an amount of entanglement scaling exponentially in the number of communicated qubits is sufficient to render any such scheme insecure. Furthermore, we show that certain schemes are secure under the assumption that the adversary has less entanglement than a given linear bound and is restricted to classical communication.
 R. König and R. Renner.
Sampling of minentropy relative to quantum knowledge.
IEEE Transactions on Information Theory, vol. 57, no. 7, pp. 47604787, July 2011. arXivLet X_{1},..., X_{n} be a sequence of n classical random variables and consider a sample of r positions selected at random. Then, except with (exponentially in r) small probability, the minentropy of the sample is not smaller than, roughly, a fraction r/n of the total minentropy of all positions X_{1},..., X_{n}, which is optimal. Here, we show that this statement, originally proven by Vadhan [LNCS, vol. 2729, Springer, 2003] for the purely classical case, is still true if the minentropy is measured relative to a quantum system. Because minentropy quantifies the amount of randomness that can be extracted from a given random variable, our result can be used to prove the soundness of locally computable extractors in a context where side information might be quantummechanical. In particular, it implies that key agreement in the boundedstorage model (using a standard sampleandhash protocol) is fully secure against quantum adversaries, thus solving a longstanding open problem.
 R. König, G. Kuperberg and B. Reichardt.
Quantum computation with TuraevViro codes.
Annals of Physics, vol. 325, no. 12, pp. 27072749, December 2010. arXivThe TuraevViro invariant for a closed 3manifold is defined as the contraction of a certain tensor network. The tensors correspond to tetrahedra in a triangulation of the manifold, with values determined by a fixed spherical category. For a manifold with boundary, the tensor network has free indices that can be associated to qudits, and its contraction gives the coefficients of a quantum errorcorrecting code. The code has local stabilizers determined by Levin and Wen. For example, applied to the genusone handlebody using the _{2} category, this construction yields the wellknown toric code. For other categories, such as the Fibonacci category, the construction realizes a nonabelian anyon model over a discrete lattice. By studying braid group representations acting on equivalence classes of colored ribbon graphs embedded in a punctured sphere, we identify the anyons, and give a simple recipe for mapping fusion basis states of the doubled category to ribbon graphs. We explain how suitable initial states can be prepared efficiently, how to implement braids, by successively changing the triangulation using a fixed fivequdit local unitary gate, and how to measure the topological charge. Combined with known universality results for anyonic systems, this provides a large family of schemes for quantum computation based on local deformations of stabilizer codes. These schemes may serve as a starting point for developing faulttolerance schemes using continuous stabilizer measurements and active errorcorrection.
 G. Alagic, S. Jordan, R. König and B. Reichardt.
Approximating TuraevViro 3manifold invariants is universal for quantum computation.
Phys. Rev. A 81, 052309 (R), October 2010. arXivThe TuraevViro invariants are scalar topological invariants of compact, orientable 3manifolds. We give a quantum algorithm for additively approximating TuraevViro invariants of a manifold presented by a Heegaard splitting. The algorithm is motivated by the relationship between topological quantum computers and (2 + 1)  D topological quantum field theories. Its accuracy is shown to be nontrivial, as the same algorithm, after efficient classical preprocessing, can solve any problem efficiently decidable by a quantum computer. Thus approximating certain TuraevViro invariants of manifolds presented by Heegaard splittings is a universal problem for quantum computation. This establishes a novel relation between the task of distinguishing nonhomeomorphic 3manifolds and the power of a general quantum computer.
 R. König and E. Bilgin.
Anyonic entanglement renormalization.
Phys. Rev. B 82, 125118, September 2010. arXivWe introduce a family of variational ansatz states for chains of anyons which optimally exploits the structure of the anyonic Hilbert space. This ansatz is the natural analog of the multiscale entanglement renormalization ansatz for spin chains. In particular, it has the same interpretation as a coarsegraining procedure and is expected to accurately describe critical systems with algebraically decaying correlations. We numerically investigate the validity of this ansatz using the anyonic golden chain and its relatives as a testbed. This demonstrates the power of entanglement renormalization in a setting with nonabelian exchange statistics, extending previous work on qudits, bosons and fermions in two dimensions.
 R. König.
Composite anyon coding and the initialization of a topological quantum computer.
Phys. Rev. A 81, 052309, May 2010. arXivSchemes for topological quantum computation are usually based on the assumption that the system is initially prepared in a specific state. In practice, this state preparation is expected to be challenging as it involves nontopological operations which heavily depend on the experimental realization and are not naturally robust against noise. Here we show that this assumption can be relaxed by using composite anyons: starting from an unknown state with reasonable physical properties, it is possible to efficiently distill suitable initial states for computation purely by braiding. This is achieved by encoding logical information in a subsystem code with gauge system corresponding to the internal degrees of freedom of composite objects.
 R. König.
Simplifying quantum double Hamiltonians using perturbative gadgets.
Quantum Information and Computation, vol. 10, no. 3, pp. 292324, March 2010. arXivPerturbative gadgets were originally introduced to generate effective klocal interactions in the lowenergy sector of a 2local Hamiltonian. Extending this idea, we present gadgets which are specifically suited for realizing Hamiltonians exhibiting nonabelian anyonic excitations. At the core of our construction is a perturbative analysis of a widely used hoppingterm Hamiltonian. We show that in the lowenergy limit, this Hamiltonian can be approximated by a certain ordered product of operators. In particular, this provides a simplified realization of Kitaev's quantum double Hamiltonians.
 R. König and S. Wehner.
A strong converse for classical channel coding using entangled inputs.
Phys. Rev. Lett. 103, 070504, August 2009. arXivA fully general strong converse for channel coding states that when the rate of sending classical information exceeds the capacity of a quantum channel, the probability of correctly decoding goes to zero exponentially in the number of channel uses, even when we allow code states which are entangled across several uses of the channel. Such a statement was previously only known for classical channels and the quantum identity channel. By relating the problem to the additivity of minimum output entropies, we show that a strong converse holds for a large class of channels, including all unital qubit channels, the ddimensional depolarizing channel and the WernerHolevo channel. This further justifies the interpretation of the classical capacity as a sharp threshold for informationtransmission.
 R. König, R. Renner and C. Schaffner.
The operational meaning of min and maxentropy.
IEEE Transactions on Information Theory, vol. 55, no. 9, pp. 43374347, September 2009. arXivWe show that the conditional minentropy H_{min}(A B) of a bipartite state is directly related to the maximum achievable overlap with a maximally entangled state if only local actions on the Bpart of are allowed. In the special case where A is classical, this overlap corresponds to the probability of guessing A given B. In a similar vein, we connect the conditional maxentropy H_{max}(A B) to the maximum fidelity of with a product state that is completely mixed on A. In the case where A is classical, this corresponds to the security of A when used as a secret key in the presence of an adversary holding B. Because min and maxentropies are known to characterize informationprocessing tasks such as randomness extraction and state merging, our results establish a direct connection between these tasks and basic operational problems. For example, they imply that the (logarithm of the) probability of guessing A given B is a lower bound on the number of uniform secret bits that can be extracted from A relative to an adversary holding B.
 R. König, B. Reichardt and G. Vidal.
Exact entanglement renormalization for stringnet models.
Phys. Rev. B 79, 195123, May 2009. arXivWe construct an explicit renormalization group (RG) transformation for Levin and Wen's stringnet models on a hexagonal lattice. The transformation leaves invariant the groundstate "fixedpoint" wave function of the stringnet condensed phase. Our construction also produces an exact representation of the wave function in terms of the multiscale entanglement renormalization ansatz (MERA). This sets the stage for efficient numerical simulations of stringnet models using MERA algorithms. It also provides an explicit quantum circuit to prepare the stringnet groundstate wave function using a quantum computer.
 R. König and G. Mitchison.
A most compendious and facile quantum de Finetti theorem.
J. Math. Phys. 50, 012105, January 2009. arXivIn its most basic form, the finite quantum de Finetti theorem states that the reduced kpartite density operator of an npartite symmetric state can be approximated by a convex combination of kfold product states. Variations of this result include Renner's ``exponential'' approximation by ``almostproduct'' states, a theorem which deals with certain triples of representations of the unitary group, and D'Cruz et al.'s result for infinitedimensional systems. We show how these theorems follow from a single, general de Finetti theorem for representations of symmetry groups, each instance corresponding to a particular choice of symmetry group and representation of that group. This gives some insight into the nature of the set of approximating states, and leads to some new results, including an exponential theorem for infinitedimensional systems.
 M. Christandl, R. König and R. Renner.
Postselection technique for quantum channels with applications to quantum cryptography.
Phys. Rev. Lett. 102, 020504, January 2009. arXivWe propose a general method for studying properties of quantum channels acting on an npartite system, whose action is invariant under permutations of the subsystems. Our main result is that, in order to prove that a certain property holds for any arbitrary input, it is sufficient to consider the special case where the input is a particular de Finettitype state, i.e., a state which consists of n identical and independent copies of an (unknown) state on a single subsystem. A similar statement holds for more general channels which are covariant with respect to the action of an arbitrary finite or locally compact group.
Our technique can be applied to the analysis of informationtheoretic problems. For example, in quantum cryptography, we get a simple proof for the fact that security of a discretevariable quantum key distribution protocol against collective attacks implies security of the protocol against the most general attacks. The resulting security bounds are tighter than previously known bounds obtained by proofs relying on the exponential de Finetti theorem [Renner, Nature Physics 3,645(2007)].  R. König and M. Wolf.
On Exchangeable Continuous Variable Systems.
J. Math. Phys. 50, 012102, January 2009. arXivWe investigate permutationinvariant continuous variable quantum states and their covariance matrices. We provide a complete characterization of the latter with respect to permutationinvariance, exchangeability and representing convex combinations of tensor power states. On the level of the respective density operators this leads to necessary criteria for all these properties which become necessary and sufficient for Gaussian states. For these we use the derived results to provide de Finettitype theorems for various distance measures.
 R. König and B. Terhal.
The Bounded Storage Model in The Presence of a Quantum Adversary.
IEEE Transactions on Information Theory, vol. 54, no. 7, pp. 749762, February 2008. arXivAn extractor is a function E that is used to extract randomness. Given an imperfect random source X and a uniform seed Y, the output E(X,Y) is close to uniform. We study properties of such functions in the presence of prior quantum information about X, with a particular focus on cryptographic applications. We prove that certain extractors are suitable for key expansion in the bounded storage model where the adversary has a limited amount of quantum memory. For extractors with onebit output we show that the extracted bit is essentially equally secure as in the case where the adversary has classical resources. We prove the security of certain constructions that output multiple bits in the bounded storage model.
 M. Christandl, R. König, G. Mitchison and R. Renner.
1 1/2 de Finetti Theorems.
Comm. Math. Phys., 273 (2), 473498, July 2007. arXivWe prove a new kind of quantum de Finetti theorem for representations of the unitary group U(d ). Consider a pure state that lies in the irreducible representation U_{+} for Young diagrams and . U_{+} is contained in the tensor product of U_{} and U_{}; let be the state obtained by tracing out U_{}. We show that is close to a convex combination of states Uv, where U is in U(d ) and v is the highest weight vector in U_{}. When U_{+} is the symmetric representation, this yields the conventional quantum de Finetti theorem for symmetric states, and our method of proof gives nearoptimal bounds for the approximation of by a convex combination of product states. For the class of symmetric Werner states, we give a second de Finettistyle theorem (our 'half' theorem); the de Finettiapproximation in this case takes a particularly simple form, involving only product states with a fixed spectrum. Our proof uses purely group theoretic methods, and makes a link with the shifted Schur functions. It also provides some useful examples, and gives some insight into the structure of the set of convex combinations of product states.
 R. König, R. Renner, A. Bariska and U. Maurer.
Small Accessible Quantum Information Does Not Imply Security.
Phys. Rev. Lett. 98, 140502, April 2007. arXivThe unconditional security of a quantum key distribution protocol is often defined in terms of the accessible information, that is, the maximum mutual information between the distributed key S and the outcome of an optimal measurement on the adversary's (quantum) system. We show that, even if this quantity is small, certain parts of the key S might still be completely insecure when S is used in applications, such as for onetime pad encryption. This flaw is due to a locking property of the accessible information: one additional (physical) bit of information might increase the accessible information by more than one bit.
 R. König and R. Renner.
A de Finetti Representation for Finite Symmetric Quantum States.
J. Math. Phys. 46, 122108, December 2005. arXivConsider a symmetric quantum state on an nfold product space, that is, the state is invariant under permutations of the n subsystems. We show that, conditioned on the outcomes of an informationally complete measurement applied to a number of subsystems, the state in the remaining subsystems is close to having product form. This immediately generalizes the socalled de Finetti representation to the case of finite symmetric quantum states.
 R. König, U. Maurer and R. Renner.
On the Power of Quantum Memory.
IEEE Transactions on Information Theory, vol. 51, no. 7, pp. 23912401, July 2005. arXivWe address the question whether quantum memory is more powerful than classical memory. In particular, we consider a setting where information about a random nbit string X is stored in r classical or quantum bits, for r < n, i.e., the stored information is bound to be only partial. Later, a randomly chosen binary question F about X is asked, which has to be answered using only the stored information. The maximal probability of correctly guessing the answer F(X) is then compared for the cases where the storage device is classical or quantum mechanical, respectively. We show that, despite the fact that the measurement of quantum bits can depend arbitrarily on the question F to be answered, the quantum advantage is negligible already for small values of the difference n  r. An implication for cryptography is that privacy amplification by application of a compression function mapping nbit strings to sbit strings (for some s < n  r), chosen publicly from a twouniversal class of hash functions, remains essentially equally secure when the adversary's memory is allowed to be r quantum rather than only r classical bits.
Other publications
 X. Ni, F. Pastawski, B. Yoshida and R. König. Preparing topologically ordered states by Hamiltonian interpolation. arXiv
 R. König and V. Scholz. Matrix product approximations to multipoint functions in twodimensional conformal field theory. arXiv
 R. König and V. Scholz. Matrix product approximations to conformal field theories. arXiv
 R. König, U. Maurer and S. Tessaro. Abstract Storage Devices,
SOSFEM 2009: Theory and Practice of Computer Science, Lecture Notes in Computer Science, Springer, vol. 5404, pp. 341352.  R. König.
de Finetti theorems for Quantum States.
PhD thesis, University of Cambridge, 2007.  R. König.
de Finetti theorems and extractors: grouptheoretic and combinatorial tools for quantum information processing.
First year report/essay, University of Cambridge, 2007.  R. König and U. Maurer.
Generalized Strong Extractors and Deterministic Privacy Amplification.
Cryptography and Coding 2005, Lecture Notes in Computer Science, Springer, vol. 3796, pp. 322339.  R. Renner and R. König.
Universally composable privacy amplification against quantum adversaries.
Theory of Cryptography 2005, Lecture Notes in Computer Science, Springer, Springer, vol. 3378, pp. 407425. arXiv  R. König, U. Maurer and R. Renner.
Privacy Amplification Secure Against an Adversary with Selectable Knowledge.
In Proceedings of 2004 IEEE International Symposium on Information Theory, 2004.  R. König and U. Maurer.
Extracting Randomness From Generalized Symbolfixing and Markov Sources.
In Proceedings of 2004 IEEE International Symposium on Information Theory, 2004.  R. König.
On the Capacity of Quantum Memory.
Diploma Thesis in theoretical physics at ETH Zurich, 2003.
CV
01/2015   assistant professor  Institute for Advanced Study and & Zentrum Mathematik, Technische Universität München 
08/2012   assistant professor  Department of Applied Mathematics and Institute for Quantum Computing, University of Waterloo 
06/2011  06/2012  postdoctoral researcher  Physics of Information/Quantum Information group, IBM Watson Research Center 
11/2007  05/2011  postdoctoral researcher  Institute for Quantum Information, California Institute of Technology (supported by an SNF fellowship starting 11/2009) 
2005  2007  Ph.D.  Department of Applied Mathematics and Theoretical Physics, University of Cambridge, UK 
2003  2005  research and teaching assistant  Institute for Theoretical Computer Science, Swiss Federal Institute of Technology (ETH), Zurich 
1998  2003  diploma (MSc.)  Theoretical Physics, ETH Zurich 