Use the coordinate convention
In this convention the Heisenberg group over a prime field has the product
The subset is an Abelian subgroup of order : the middle coordinate in a product is , which is symmetric in the factors. Also lies in . The map is a surjective group homomorphism to the additive group of , with kernel of a group homomorphism . Hence is a normal subgroup of subgroup index , and its left cosets are exactly the level sets of .
For odd , an explicit group isomorphism from to the additive group is
The term in matrix multiplication cancels the cross term in . Thus is an elementary abelian group, isomorphic to .
In the Heisenberg group over a commutative ring with , the subset is an Abelian subgroup of group order 16. Its product has central coordinate , symmetric in the two factors. Its inverse element is . The map is a surjective group homomorphism to the additive group of , with kernel of a group homomorphism . Thus is a normal subgroup and has four cosets in the 64-element group.
Unlike the odd-prime case, division by two is unavailable. In fact take and . Then , where the binomial coefficient is computed as an integer before reduction modulo four. Hence and has element order eight. The element has element order two and is not a power of : the powers with outer coordinates two have central coordinates one or three. Their generated subgroups intersect trivially, so the 16-element Abelian group is the direct product of groups .
Finite abelian subgroup of the Möbius group Created 2026-10-06 Updated 2026-10-14
A finite abelian subgroup of the Möbius group is cyclic or isomorphic to . If it contains an element of order greater than two, conjugate that element's two fixed points to . Every commuting map must preserve these points individually: an interchange would conjugate the element to its inverse. All maps are then scalings, forming a cyclic finite subgroup of . If every nonidentity element has order two, choose one with fixed points ; the subgroup acts on this pair with image of size at most two and kernel contained in . Its size is therefore at most four, giving the asserted possibilities.
Use the product from part (ii). Move each selected element of each small set to the left, conjugating every approximate-group factor that it crosses. For each tuple , the corresponding part of the product is therefore contained in
where every is a conjugate subset of some . Conjugation preserves cardinality, the approximation parameter, and the property that the generated subgroup is abelian. The conjugating elements belong to , so after enlarging the implicit constant.
The number of tuples is at most
These translated products cover , so one has size at least the reciprocal fraction of . For that tuple, put . Then
where , and each is a -approximate group generating an abelian subgroup.
Cosets and Lagrange. A left coset is . The left cosets of a subgroup partition a group, each with elements. Lagrange's theorem states for a finite group, so every subgroup order divides the group order.
The 64-element group. Work in the commutative ring , which has zero divisors. Denote the displayed lower triangular matrix by , where are its three entries below the diagonal. Direct matrix multiplication gives
All arithmetic is modulo four, so the set is closed. Associativity comes from matrix multiplication, the identity element is , and
The formula works in either multiplication order and requires no division. Hence these matrices form a group of order . This is the lower triangular version of the Heisenberg group over a commutative ring.
The abelian subgroup. If , write . Then
The identity is and the inverse is , proving an abelian subgroup. Its two independent entries give and , in accordance with Lagrange's theorem. This is the abelian plane subgroup of the Heisenberg group modulo four.
More explicitly, is a surjective group homomorphism to the additive group of , with kernel . The four left cosets are exactly the four sets with fixed , ; representatives are . Thus is also a normal subgroup.
Matrices squaring to the identity. The product formula gives
The first and third coordinates vanish only when . Then modulo four, so the middle coordinate vanishes exactly when . Therefore the complete set is
It is a subgroup: multiplying two such elements keeps all three entries even, and their cross term vanishes modulo four, so the product simply adds the three even coordinates. The identity is included and each element is its own inverse. In fact is isomorphic to the direct product of groups . The seven nonidentity elements are involutions.
Finally, the last subset in the PDF is defined by , with no restriction on . It has elements, which cannot be a subgroup because does not divide . It also excludes the identity element. Thus
Cosets and counting. A left coset of a subgroup in a group is . The left cosets partition and each has elements. Lagrange's theorem states that for a finite group, ; in particular, the subgroup order divides the group order.
The matrix group. Work throughout in the finite field , so every nonzero entry has a multiplicative inverse. Denote a matrix by , with . Ordinary matrix multiplication, interpreted using modular arithmetic, gives
Its diagonal entries remain nonzero, proving closure. Associativity is inherited from matrix multiplication, is the identity element, and
This lies in the same set and multiplication checks the inverse in either order. Thus these matrices form a group. There are four choices each for and and five for , giving .
The subgroup. Write . Then
It contains the identity , is closed, and has inverse . Interchanging the two factors leaves the product unchanged because multiplication in is commutative. Therefore is an abelian subgroup, with
Equivalently is isomorphic to by , which also explains its abelian property. Its order divides , verifying Lagrange's theorem.
There are five distinct left cosets. Representatives can be taken as , : indeed
Every matrix lies in exactly the coset specified by this unique .
Elements whose square is the identity. Squaring gives
Thus and . For equal signs, in , so . For opposite signs, and all five values work. The complete set is therefore
It contains elements, including the identity; the other eleven are involutions. Since does not divide , Lagrange's theorem proves that this set is not a subgroup.
Two elements are conjugate group elements if for some . The conjugacy class of is . Conjugacy is an equivalence relation: it is reflexive using , symmetric by replacing with , and transitive because
Thus the classes partition the group: every element belongs to its own class, and any two classes that intersect are equal. This proves that every element belongs to exactly one class.
If is Abelian, then , so every class is a singleton. In general the elements whose classes are singletons are precisely those commuting with every group element. Thus the center of a group is
It contains . If , then commutes with every , since does and does. The subgroup test therefore proves that is a subgroup. Any two of its elements commute with each other, so it is an abelian subgroup.
For the square centred at the origin with vertices , put
The dihedral group consists of and , . Its eight actions and their matrices are
These exhaust the symmetries: the image of one vertex has four choices and the image of an adjacent vertex has two choices, determining the entire square. For an explicit pair of nonconjugate elements take and . Both have order two, but their determinants are and . A similarity transformation preserves the determinant, so and are not conjugate.
To find the centre, use . A rotation commutes with exactly when , so is even. No reflection commutes with , since while , and . Therefore
The identity commutes with every group element, so it lies in the center of a group. If are central and , then implies . Consequently
Thus is central. The subgroup test proves
Equivalently, the centre is nonempty, closed under products, and closed under inverses. This proof does not require finiteness. In fact the centre is an Abelian subgroup, and it is normal because for each central element.
Perform the product and inverse formulas from part (b) in the commutative ring . They involve only addition, multiplication and negatives, so closure and inverses remain valid; no division by a nonunit is needed. Associativity again comes from matrix multiplication, and remains the identity. The Heisenberg group over a commutative ring therefore has
These are residues modulo four, not arithmetic in the finite field of four elements.
For the additional subgroup task, write an element of as . Its product and inverse are
Both remain in , and the product is unchanged on exchanging the factors because . The identity is included, so is an Abelian subgroup. There are four independent choices each for , giving
Thus there are four distinct left cosets. Explicitly the surjective group homomorphism has kernel ; the four cosets are the level sets of that difference, with representatives , . This is the Abelian plane subgroup of the Heisenberg group modulo four.
A member of is . The multiplication law from part (a) becomes
It stays in and is unchanged when the two factors are exchanged, since . The identity lies in , and also lies in . Thus is an Abelian subgroup, namely the Abelian plane subgroup of a finite Heisenberg group in this coordinate convention.
There are five choices each for , so
This verifies Lagrange's theorem: the subgroup order divides the group order, and the number of distinct left cosets is five.
Explicitly, the map is a surjective group homomorphism to the additive group of , by the product formula. Its kernel of a group homomorphism is . Thus is even a normal subgroup; the five left cosets are the level sets for , with representatives . Each contains 25 elements, providing a direct count as well.
The center of a group contains . If lie in the center, then for every ,
It is therefore closed under the group operation and inverse elements, and inherits associativity, proving it is a subgroup. Each of its elements commutes with every element of , in particular with every other central element. Hence
Thus the center is an abelian subgroup.
Stabilizer code Created 2026-09-24 Updated 2026-10-14
A stabilizer code is the common eigenspace of a stabilizer group , an abelian subgroup of the Pauli group excluding . Choose independent stabilizer generators on physical qubits. They are commuting Hermitian operators, each squaring to . The stabilizer subspace and its orthogonal projector are
The stabilizer-projector formula gives , so logical qubits remain. Independent here means that no nonempty product of the chosen stabilizer generators is . Excluding is necessary: a vector cannot simultaneously be fixed by and unless it is zero.
For the three-qubit bit-flip repetition code, take and , with the Pauli Z gate on site and identities elsewhere. The stabilizer group is . Both stabilizer generators have eigenvalue exactly on the span of and , giving dimensions for one logical qubit. A projective measurement of these checks distinguishes four orthogonal two-dimensional sectors rather than eight individual computational basis states.
A Pauli error that anticommutes with a stabilizer generator changes that check's sign, producing an error syndrome. A Pauli operator commuting with every check can still act on the logical qubits; the centralizer of a stabilizer group describes these possibilities. Thus the number of checks determines the encoded dimension, while the quantum code distance determines protection against arbitrary local errors. The five-qubit error correcting code, for instance, has four stabilizer generators and quantum code distance three; the three-qubit bit-flip repetition code has two checks but quantum code distance one because a single phase flip is unflagged. [ref].