Introduction

A homogeneous polynomial p∈R[x1,…,xm]p \in\mathbb{R}[x_1,\ldots,x_m] of degree d≥1d \ge1 is hyperbolic with respect to e∈Rme \in\mathbb{R}^m if p(e)≠0p(e) \ne0 and every root of t↦p(te−x)t \mapsto p(te-x) is real for every x∈Rmx \in\mathbb{R}^m. Write these roots, with multiplicity, as λ1(x),…,λd(x)\lambda_1(x),\ldots,\lambda_d(x). The closed hyperbolicity cone is

Λ+(p,e)={x∈Rm:λj(x)≥0 for 1≤j≤d}.\Lambda_+(p,e)=\{x \in\mathbb{R}^m:\lambda_j(x)\ge0\text{ for }1\le j\le d\}.

We write SN\mathbb{S}^N for the real symmetric N×NN \times N matrices and A⪰0A \succeq0 (respectively, A≻0A \succ0) for positive semidefiniteness (respectively, positive definiteness). A cone is spectrahedral if it has the form

K={x∈Rm:L(x)⪰0},L(x)=∑i=1mxiAi,Ai∈SN,(1)K=\{x \in\mathbb{R}^m:L(x)\succeq0\},\qquad L(x)=\sum_{i=1}^{m}x_iA_i,\quad A_i\in\mathbb{S}^N, \tag*{(1)}

for some finite N≥1N \ge1. The geometric Generalized Lax conjecture asserts that every hyperbolicity cone is spectrahedral. We give a counterexample.

The explicit polynomial

All indices in {1,2,3}\{1,2,3\} in the following construction are cyclic. For z,y∈R3z,y \in\mathbb{R}^{3}, let

b(z,y)=∑i=13zi2yi2−2∑1≤i<j≤3ziyizjyj+∑i=13zi2yi+12.(2)b(z,y)=\sum_{i=1}^{3}z_i^{2}y_i^{2}-2\sum_{1\le i<j\le3}z_i y_i z_j y_j+\sum_{i=1}^{3}z_i^{2}y_{i+1}^{2}. \tag*{(2)}

This is the coefficient-one Choi–Lam biquadratic form [4], Section 4. Define Q(y)∈S3Q(y) \in\mathbb{S}^{3} by

Q(y)ii=yi2+yi+12,Q(y)ij=−yiyj(i≠j).Q(y)_{ii}=y_i^{2}+y_{i+1}^{2},\qquad Q(y)_{ij}=-y_i y_j\quad(i\ne j).

so that b(z,y)=zTQ(y)zb(z,y)=z^{\mathsf{T}}Q(y)z. For a∈Ra\in\mathbb{R}, r∈R3r\in\mathbb{R}^{3} and T∈S3T\in\mathbb{S}^{3}, define the linear map Φy:S4→S4\Phi_y:\mathbb{S}^{4}\to\mathbb{S}^{4} by

Φy(arTrT)=(tr⁡(Q(y)T)−rTQ(y)−Q(y)raQ(y)).(3)\Phi_y\begin{pmatrix}a&r^{\mathsf{T}}\\r&T\end{pmatrix} = \begin{pmatrix} \operatorname{tr}(Q(y)T)&-r^{\mathsf{T}}Q(y)\\ -Q(y)r&aQ(y) \end{pmatrix}. \tag*{(3)}

The dependence on yy is homogeneous quadratic. If adj⁡X\operatorname{adj}X denotes the adjugate of XX, set

p(X,Z,y)=det⁡((det⁡X)Z−Φy(adj⁡X)),(X,Z,y)∈S4×S4×R3.(4)p(X,Z,y)=\det\bigl((\det X)Z-\Phi_y(\operatorname{adj}X)\bigr),\qquad(X,Z,y)\in\mathbb{S}^{4}\times\mathbb{S}^{4}\times\mathbb{R}^{3}. \tag*{(4)}

This formula is polynomial even when XX is singular. The ambient space has dimension 10+10+3=2310+10+3=23.

Theorem 1.1. The polynomial (1.4)(1.4) is homogeneous of degree 20 and hyperbolic with respect to e=(I4,I4,0)e=(I_4,I_4,0), with p(e)=1p(e)=1. Its closed hyperbolicity cone K=Λ+(p,e)K=\Lambda_{+}(p,e) is not spectrahedral: for every finite N≥1N\ge1 and every real linear map L:S4×S4×R3→SNL:\mathbb{S}^{4}\times\mathbb{S}^{4}\times\mathbb{R}^{3}\to\mathbb{S}^{N},

K≠{(X,Z,y):L(X,Z,y)⪰0}.K\ne\{(X,Z,y):L(X,Z,y)\succeq0\}.

The conclusion concerns the cone itself, so it allows every possible defining pencil and every finite matrix size. The compact formula for pp is convenient for the proof, but one determinant factor can be removed.

Corollary 1.2. The quotient q=p/det⁡Xq=p/\det X extends to a homogeneous polynomial of degree 16 in the same 23 variables. It is hyperbolic with respect to ee, with q(e)=1q(e)=1, and Λ+(q,e)=K\Lambda_{+}(q,e)=K. In particular, its closed hyperbolicity cone is not spectrahedral.

We prove the degree reduction in Section 7, after the obstruction argument. We make no claim that the dimension or degree is minimal. The real symmetric convention also covers Hermitian pencils: for a Hermitian matrix H=A+iBH=A+iB, positivity is equivalent to positivity of the real symmetric matrix (A−BBA)\begin{pmatrix}A&-B\\B&A\end{pmatrix}.

Historical context

Gårding’s theory establishes the convexity of hyperbolicity cones [6]. The original Lax conjecture asks for a definite determinantal representation of homogeneous hyperbolic polynomials in three variables [12]. Helton and Vinnikov proved the corresponding definite determinantal representation theorem [9]; Lewis, Parrilo, and Ramana established its equivalence with Lax’s formulation [13]. In higher dimension, Brändén constructed a real-zero polynomial none of whose positive powers admits a definite determinantal representation [2]. That obstruction does not exclude a different determinant, with additional factors, from defining the same cone. The geometric conjecture concerns this remaining possibility. Kummer exhibited the distinction concretely: the cone of the specialized Vámos polynomial has a 7×77 \times7 representation, although no positive power of that polynomial has a definite determinantal representation [10]. Raghavendra, Ryder, Srivastava, and Weitz proved exponential lower bounds on the matrix size of spectrahedral representations for suitable hyperbolicity cones [16]. Recent positive results include Netzer’s theorem for hyperbolic cubics in five variables [14].

Kummer and Netzer prove spectrahedrality for cones of strictly hyperbolic polynomials [11]. Here strictly hyperbolic means that p(te−x)p(te-x) has distinct roots whenever x∉ℜx \notin\Re. The polynomial (1.4) fails this hypothesis: at w=(I4,0,0)∉ℜw=(I_4,0,0) \notin\Re it gives

p(te−w)=(t−1)16t4p(te-w)=(t-1)^{16}t^4

For the reduced polynomial of Corollary 1.2, the same line gives q(te−w)=(t−1)12t4q(te-w)=(t-1)^{12}t^4. Thus neither defining polynomial satisfies the strict-case hypothesis.

A spectrahedral shadow is a linear image of a set defined by an affine real symmetric linear matrix inequality. Netzer and Sanyal proved that a hyperbolicity cone is a spectrahedral shadow when every nonzero boundary point is a smooth point of the defining polynomial [15]. Our result concerns a direct representation in the original variables; it makes no assertion about representations using auxiliary variables.

The scalar ingredient is the coefficient-one Choi–Lam biquadratic form [4], which reduces the coefficient of the extra cyclic squared monomials from two in Choi’s earlier nonnegative form [3] to one. Its inability to dominate a nonzero bilinear square follows from the extremality proved in [4]; we give a short proof of precisely this property. It is called weak extremality by Blekherman, Raiţă, Shankar, and Sinn [1], whose characterization uses Taylor expansions of dominated squares at zeros [1]. The correspondence between nonnegative biquadratic forms and positive maps on real symmetric matrices is classical; see [8]. Positive maps have also been used to obtain certificates of conic polynomial stability [5]. Here the construction turns the scalar obstruction into an obstruction to every finite pencil describing one hyperbolicity cone. A related general strategy appears in Scheiderer’s local sums-of-squares obstructions to spectrahedral shadows [17]. Our proof extracts bilinear square minors from a differentiated operator-norm identity; it does not invoke a criterion for shadows.

González Nevado states a positive solution of the geometric conjecture in [7]. Appendix A records a counterexample to the path-containment assertion used in that argument. The construction and proof in the present paper are independent of that comparison.

Proof strategy

The scalar obstruction is particularly rigid: bb is nonnegative and nonzero, but every bilinear form ℓ\ell satisfying ℓ(z,y)2≤b(z,y)\ell(z,y)^2 \le b(z,y) for all z,yz,y is zero. Section 2 gives a short proof using zeros and curves along which bb vanishes to fourth order.

The map Φy\Phi_y translates this form into a matrix inequality. In Section 3 we prove hyperbolicity and identify the slice of KK with X≻0X \succ0 as

Z⪰Φy(X−1).Z \succeq\Phi_y(X^{-1}).

The remaining argument assumes an arbitrary pencil defining KK and extracts a bilinear square dominated by bb. First, Section 4 rescales the pencil along (X,s2Z,sy)(X,s^2Z,sy) and obtains an equivalent block matrix inequality. Section 5 then sends X−1X^{-1} and Z−1Z^{-1} toward rank-one projections; the resulting comparison yields an exact operator-norm identity for kernel projections of the pencil blocks. These projections are parametrized by the unit sphere in R4\mathbb{R}^4. Finally, Section 6 differentiates one kernel projection on a neighborhood of constant rank in that sphere. At a suitable base point, the three-dimensional tangent space can be identified with all the zz-variables, so this local identity controls bb for every zz and yy. Each entry of the resulting matrix is a bilinear form whose square is bounded by bb, giving a contradiction.

The mechanism connecting the biquadratic form to the geometry of the cone is the rescaling and subsequent first variation of these kernel projections. It applies to an arbitrary hypothetical pencil without comparing its determinant with pp. All matrix norms below are Euclidean operator norms, denoted by ∥⋅∥op\|\cdot\|_{\mathrm{op}}; vector norms are Euclidean.

A biquadratic form with no dominated square

The geometric argument will produce bilinear forms whose squares are bounded by the Choi–Lam form bb in (2). We prove directly the particular consequence of its classical extremality [4], Theorem 4.4 that the geometric argument needs: every such bilinear form must vanish. This property is also called weak extremality [1], Definition 2.7.

Lemma 2.1. The form b:R3×R3→Rb : \mathbb{R}^3 \times\mathbb{R}^3 \to\mathbb{R} defined in (2) is nonnegative and nonzero. If a real bilinear form ℓ:R3×R3→R\ell: \mathbb{R}^3 \times\mathbb{R}^3 \to\mathbb{R} satisfies

ℓ(z,y)2≤b(z,y)for every z,y∈R3,\ell(z,y)^2 \le b(z,y) \qquad\text{for every } z,y \in\mathbb{R}^3,

then ℓ=0\ell= 0.

Proof. Put ai=zi2a_i=z_i^2, with indices read cyclically modulo 3. The matrix of b(z,y)b(z,y) as a quadratic form in yy is

M(z)=(a1+a3−z1z2−z1z3−z1z2a2+a1−z2z3−z1z3−z2z3a3+a2).M(z)=\begin{pmatrix} a_1+a_3 & -z_1z_2 & -z_1z_3\\ -z_1z_2 & a_2+a_1 & -z_2z_3\\ -z_1z_3 & -z_2z_3 & a_3+a_2 \end{pmatrix}.

Its diagonal entries are nonnegative. Its three principal minors of order two are

det⁡M(z)[{i,i+1}]=ai2+ai−1(ai+ai+1)≥0,i=1,2,3,\det M(z)[\{i,i+1\}]=a_i^2+a_{i-1}(a_i+a_{i+1})\ge0,\qquad i=1,2,3,

where the brackets denote a principal submatrix. Finally,

det⁡M(z)=a12a2+a22a3+a32a1−3a1a2a3≥0\det M(z)=a_1^2a_2+a_2^2a_3+a_3^2a_1-3a_1a_2a_3\ge0

by the arithmetic–geometric mean inequality. All principal minors are therefore nonnegative, so M(z)⪰0M(z)\succeq0 and b(z,y)≥0b(z,y)\ge0. For the standard coordinate vectors e1,e2,e3e_1,e_2,e_3 of R3\mathbb{R}^3, we have b(e1,e1)=1b(e_1,e_1)=1.

Now write ℓ(z,y)=∑i,jcijziyj\ell(z,y)=\sum_{i,j}c_{ij}z_i y_j and assume the stated bound. Zeros will eliminate the off-diagonal coefficients; fourth-order vanishing along curves will eliminate the diagonal coefficients. At every zero of bb, the form ℓ\ell vanishes. In particular,

b(ei,ei−1)=0⟹ci,i−1=0.b(e_i,e_{i-1})=0 \quad\Longrightarrow\quad c_{i,i-1}=0.

For each sign vector σ∈{−1,1}3\sigma\in\{-1,1\}^{3}, we also have b(σ,σ)=3−6+3=0b(\sigma,\sigma)=3-6+3=0, and hence

0=∑icii+∑i<j(cij+cji)σiσj.0=\sum_i c_{ii}+\sum_{i<j}(c_{ij}+c_{ji})\sigma_i\sigma_j.

Multiplying by σpσq\sigma_p\sigma_q and averaging over the eight sign vectors gives cpq+cqp=0c_{pq}+c_{qp}=0 for every p<qp<q. Together with ci,i−1=0c_{i,i-1}=0, these identities force all off-diagonal entries to vanish. Thus ℓ(z,y)=∑iciziyi\ell(z,y)=\sum_i c_i z_i y_i for some real cic_i.

For a cyclic index ii and s∈Rs\in\mathbb{R}, set

z=ei+sei−1,y=ei−1+sei.z=e_i+se_{i-1},\qquad y=e_{i-1}+se_i.

Direct substitution gives

b(z,y)=2s2−2s2+s4=s4,ℓ(z,y)=s(ci+ci−1).b(z,y)=2s^2-2s^2+s^4=s^4,\qquad\ell(z,y)=s(c_i+c_{i-1}).

For s≠0s\ne0, the bound implies (ci+ci−1)2≤s2(c_i+c_{i-1})^2\le s^2. Letting s→0s\to0 yields ci+ci−1=0c_i+c_{i-1}=0 for all three indices. These equations force c1=c2=c3=0c_1=c_2=c_3=0, proving the lemma.

Hyperbolicity and two cone slices

We first prove that the polynomial in (4) is hyperbolic. We then identify the two slices of its closed cone that will constrain any representing pencil.

For u=(u0,u′)u=(u_0,u') and v=(v0,v′)v=(v_0,v') in R4\mathbb{R}^4, the block formula []( #eq:1.3) gives

uTΦy(vvT)u=(v0u′−u0v′)TQ(y)(v0u′−u0v′)=b(v0u′−u0v′,y).(5)u^{\mathsf T}\Phi_y(vv^{\mathsf T})u=(v_0u'-u_0v')^{\mathsf T}Q(y)(v_0u'-u_0v')=b(v_0u'-u_0v',y). \tag*{(5)}

Indeed, the three terms on expanding the middle expression are v02u′TQ(y)u′v_0^2u'^{\mathsf T}Q(y)u', −2u0v0u′TQ(y)v′-2u_0v_0u'^{\mathsf T}Q(y)v', and u02v′TQ(y)v′u_0^2v'^{\mathsf T}Q(y)v', exactly the terms from the block formula. Lemma 2.1 therefore implies that Φy(vvT)⪰0\Phi_y(vv^{\mathsf T})\succeq0. Every positive semidefinite real symmetric matrix is a nonnegative linear combination of such rank-one matrices. Thus Φy\Phi_y is a positive linear map: it preserves positive semidefiniteness, and hence the order ⪯\preceq. The same formula also gives

Φsy=s2Φy(s∈R),(6)\Phi_{sy}=s^2\Phi_y\qquad(s\in\mathbb{R}), \tag*{(6)}

so in particular Φ0=0\Phi_0=0 and Φ−y=Φy\Phi_{-y}=\Phi_y. This rank-one verification is the real-symmetric positive-map correspondence for biquadratic forms [8] applied to the explicit map []( #eq:1.3).

Proposition 3.1. The polynomial pp in []( #eq:1.4) is homogeneous of degree 20 on S4×S4×R3\mathbb{S}^4\times\mathbb{S}^4\times\mathbb{R}^3, a real vector space of dimension 23. It satisfies p(e)=1p(e)=1 and is hyperbolic with respect to e=(I4,I4,0)e=(I_4,I_4,0).

Proof. Each entry of (det⁡X)Z−Φy(adj⁡X)(\det X)Z-\Phi_y(\operatorname{adj}X) is homogeneous of degree 5: the adjugate has degree 3, and Φy\Phi_y is quadratic in yy. Taking its 4×44\times4 determinant gives a homogeneous polynomial of degree 20. Since Φ0=0\Phi_0=0, evaluation at ee gives p(e)=1p(e)=1, so this polynomial is nonzero. The dimension is 10+10+3=2310+10+3=23.

Extend Φy\Phi_y complex linearly to complex symmetric matrices. For invertible XX, real or complex, linearity and adj⁡X=(det⁡X)X−1\operatorname{adj}X=(\det X)X^{-1} give

p(X,Z,y)=(det⁡X)4det⁡(Z−Φy(X−1)).(7)p(X,Z,y)=(\det X)^4\det\left(Z-\Phi_y(X^{-1})\right). \tag*{(7)}

The adjugate formula remains the definition at singular XX.

Fix real symmetric XX, ZZ and real yy, and let t=a+iηt=a+i\eta with η>0\eta>0. Orthogonal diagonalization of XX gives

Im⁡(tI4−X)−1=−η((aI4−X)2+η2I4)−1≺0.\operatorname{Im}(tI_4-X)^{-1}=-\eta\left((aI_4-X)^2+\eta^2I_4\right)^{-1}\prec0.

For a complex symmetric matrix, the entrywise imaginary part equals the Hermitian imaginary part (A−A∗)/(2i)(A-A^*)/(2i) and is real symmetric. Complex linearity and positivity of Φ−y\Phi_{-y} consequently show that

H=tI4−Z−Φ−y((tI4−X)−1)H=tI_4-Z-\Phi_{-y}\left((tI_4-X)^{-1}\right)

satisfies Im⁡H⪰ηI4≻0\operatorname{Im}H\succeq\eta I_4\succ0.

Such an HH is invertible: if Hw=0Hw=0 for a nonzero complex vector ww, then 0=Im⁡(w∗Hw)=w∗(Im⁡H)w>00=\operatorname{Im}(w^*Hw)=w^*(\operatorname{Im}H)w>0. Also tI4−XtI_4-X is invertible. Equation (7) therefore implies p(te−(X,Z,y))≠0p(te-(X,Z,y))\ne0. The coefficients of this polynomial in tt are real, so conjugation also excludes roots in the lower half-plane. Finally, its leading coefficient is p(e)=1p(e)=1 by homogeneity; it has degree 20 for every real input. All its roots are therefore real, as required.

Proposition 3.2. Let K=Λ+(p,e)K=\Lambda_+(p,e). For real symmetric XX, ZZ and y∈R3y\in\mathbb{R}^3,

X≻0:(X,Z,y)∈K ⟺ Z⪰Φy(X−1),(8)X\succ0:\qquad(X,Z,y)\in K\ \Longleftrightarrow\ Z\succeq\Phi_y(X^{-1}), \tag*{(8)}
(X,Z,0)∈K ⟺ X⪰0 and Z⪰0.(9)(X,Z,0)\in K\ \Longleftrightarrow\ X\succeq0\ \text{and}\ Z\succeq0. \tag*{(9)}

Moreover, ee lies in the interior of KK in the full ambient space.

Proof. If λ1(x),…,λ20(x)\lambda_1(x),\ldots,\lambda_{20}(x) are the roots of t↦p(te−x)t\mapsto p(te-x), homogeneity gives

p(x+te)=∏j=120(t+λj(x)).p(x+te)=\prod_{j=1}^{20}(t+\lambda_j(x)).

Thus x∈Kx\in K if and only if p(x+te)≠0p(x+te)\ne0 for every real t>0t>0. The strict inequality on tt allows zero roots and hence includes the boundary of KK.

Suppose X≻0X\succ0 and set, for t≥0t\geq0,

F(t)=Z+tI4−Φy((X+tI4)−1).F(t)=Z+tI_4-\Phi_y\left((X+tI_4)^{-1}\right).

If F(0)⪰0F(0)\succeq0, order preservation yields

F(t)=F(0)+tI4+Φy(X−1−(X+tI4)−1)⪰tI4≻0(t>0).F(t)=F(0)+tI_4+\Phi_y\left(X^{-1}-(X+tI_4)^{-1}\right)\succeq tI_4\succ0\qquad(t>0).

Equation (7) then shows that there is no positive root, so (X,Z,y)∈K(X,Z,y)\in K.

Conversely, if F(0)⪰̸0F(0)\not\succeq0, its least eigenvalue is negative. For t>0t>0, positivity gives

0⪯Φy((X+tI4)−1)⪯t−1Φy(I4).0\preceq\Phi_y\left((X+tI_4)^{-1}\right)\preceq t^{-1}\Phi_y(I_4).

Consequently F(t)≻0F(t)\succ0 for all sufficiently large tt. Continuity of its least eigenvalue gives a t>0t>0 at which F(t)F(t) is singular. Since X+tI4≻0X+tI_4\succ0, Equation (7) now gives a positive root of p((X,Z,y)+te)p((X,Z,y)+te). This proves (8) in both directions, including equality in the matrix inequality.

When y=0y=0, the polynomial definition directly gives

p(te−(X,Z,0))=det⁡(tI4−X)4det⁡(tI4−Z),p(te-(X,Z,0))=\det(tI_4-X)^4\det(tI_4-Z),

also for singular XX and ZZ. Its roots are the eigenvalues of XX, each repeated four times, and the eigenvalues of ZZ. They are all nonnegative exactly when both matrices are positive semidefinite. This proves (9).

Finally, X≻0X\succ0 and Z−Φy(X−1)≻0Z-\Phi_y(X^{-1})\succ0 define an open subset of the full ambient space. It contains ee and, by (8), is contained in KK. Thus ee is an interior point.

What a semidefinite representation would imply

The two slices in Proposition 3.2 constrain every pencil representing KK. We now turn those constraints into an exact block matrix inequality whose off-diagonal block is linear in yy. A positive linear map preserves positive semidefiniteness; it is called unital if it sends the identity to the identity.

Proposition 4.1. Let K=Λ+(p,(I4,I4,0))K = \Lambda_+(p,(I_4,I_4,0)) for the polynomial in (4). Suppose that KK admits a representation by a finite homogeneous real symmetric linear pencil. Then there are integers a,c≥1a,c \ge1, positive linear maps

D:S4⟶Sa,E:S4⟶Sc,D(I4)=Ia,E(I4)=Ic,D:\mathbb{S}^4 \longrightarrow\mathbb{S}^a,\qquad E:\mathbb{S}^4 \longrightarrow\mathbb{S}^c,\qquad D(I_4)=I_a,\qquad E(I_4)=I_c,

and a linear map B:R3⟶Ra×cB:\mathbb{R}^3 \longrightarrow\mathbb{R}^{a\times c} such that, for every X≻0X \succ0, Z∈S4Z \in\mathbb{S}^4 and y∈R3y \in\mathbb{R}^3,

Z⪰Φy(X−1)⟺E(Z)⪰B(y)TD(X)−1B(y).(10)Z \succeq\Phi_y(X^{-1}) \quad\Longleftrightarrow\quad E(Z) \succeq B(y)^\mathsf{T}D(X)^{-1}B(y). \tag*{(10)}

Proof. Write the hypothetical pencil as

L(X,Z,y)=L1(X)+L2(Z)+L3(y).L(X,Z,y)=L_1(X)+L_2(Z)+L_3(y).

We first remove the pencil’s common kernel and normalize two positive blocks. We then rescale the pencil and prove that its limit represents the same inequality.

Compression and normalization. We use the elementary fact that

A+H⪰0,A−H⪰0⟹ker⁡A⊆ker⁡H.A+H\succeq0,\quad A-H\succeq0\quad\Longrightarrow\quad\ker A\subseteq\ker H.

Indeed, if w∈ker⁡Aw\in\ker A, the two nonnegative quadratic forms on ww sum to zero. A positive semidefinite matrix annihilates every vector on which its quadratic form vanishes, so both (A+H)w(A+H)w and (A−H)w(A-H)w are zero.

Since ee is interior to KK, for every ambient vector xx there is an ε>0\varepsilon>0 with L(e)±εL(x)⪰0L(e)\pm\varepsilon L(x)\succeq0. The preceding fact shows that ker⁡L(e)\ker L(e) is a common kernel of the whole pencil. Compressing to its orthogonal complement preserves the represented cone and makes L(e)≻0L(e)\succ0. This complement is nonzero: otherwise the pencil would vanish identically, whereas (−I4,I4,0)∉K(-I_4,I_4,0)\notin K by (9).

The same slice shows that L1L_1 and L2L_2 are positive maps. Set U=ker⁡L1(I4)U=\ker L_1(I_4). Positivity at I4±εXI_4\pm\varepsilon X, for small ε>0\varepsilon>0, and the same kernel argument show that every L1(X)L_1(X) annihilates UU. Thus, in U⊥⊕UU^\perp\oplus U,

L1(X)=(D(X)000).L_1(X)= \begin{pmatrix} D(X) & 0\\ 0 & 0 \end{pmatrix}.

Both summands are nonzero. If U⊥=0U^\perp=0, then L1=0L_1=0 and the pencil accepts (−I4,I4,0)(-I_4,I_4,0), contradicting (9). If U=0U=0, then L1(I4)≻0L_1(I_4)\succ0, so L1(I4)−εL2(I4)≻0L_1(I_4)-\varepsilon L_2(I_4)\succ0 for sufficiently small ε>0\varepsilon>0. This would accept (I4,−εI4,0)(I_4,-\varepsilon I_4,0), again contradicting that slice.

Let a=dim⁡U⊥a=\dim U^\perp, c=dim⁡Uc=\dim U, and let E(Z)E(Z) be the lower diagonal block of L2(Z)L_2(Z). Both DD and EE are positive maps. Moreover, D(I4)≻0D(I_4)\succ0 by the definition of UU, and E(I4)≻0E(I_4)\succ0 because it is the compression of L(e)≻0L(e)\succ0 to UU. Apply the fixed block diagonal congruence

diag⁡(D(I4)−1/2,E(I4)−1/2)\operatorname{diag}\left(D(I_4)^{-1/2},E(I_4)^{-1/2}\right)

and retain the notation for the resulting blocks. We now have D(I4)=IaD(I_4)=I_a and E(I4)=IcE(I_4)=I_c.

Rescaling the pencil. Write the other blocks as

L2(Z)=(F(Z)C(Z)C(Z)TE(Z)),L3(y)=(A(y)B(y)B(y)TG(y)).L_2(Z)=\begin{pmatrix} F(Z) & C(Z) \\ C(Z)^{\mathsf T} & E(Z) \end{pmatrix}, \qquad L_3(y)=\begin{pmatrix} A(y) & B(y) \\ B(y)^{\mathsf T} & G(y) \end{pmatrix}.

Fix yy and put Z0=Φy(I4)Z_0=\Phi_y(I_4). By (8) and Φsy=s2Φy\Phi_{sy}=s^2\Phi_y, the point (I4,s2Z0,sy)(I_4,s^2Z_0,sy) lies in KK for every real ss. Its lower pencil block therefore satisfies

s2E(Z0)+sG(y)⪰0(s∈R).s^2E(Z_0)+sG(y)\succeq0 \qquad(s\in\mathbb{R}).

Dividing by ∣s∣\lvert s\rvert and taking limits through positive and negative ss gives G(y)⪰0G(y)\succeq0 and −G(y)⪰0-G(y)\succeq0. Hence G(y)=0G(y)=0.

For fixed X≻0X\succ0, ZZ and yy, and any real s≠0s\ne0, congruence of L(X,s2Z,sy)L(X,s^2Z,sy) by diag⁡(Ia,s−1Ic)\operatorname{diag}(I_a,s^{-1}I_c) gives

Ms(X,Z,y)=(D(X)+sA(y)+s2F(Z)B(y)+sC(Z)B(y)T+sC(Z)TE(Z)).(11)M_s(X,Z,y)=\begin{pmatrix} D(X)+sA(y)+s^2F(Z) & B(y)+sC(Z) \\ B(y)^{\mathsf T}+sC(Z)^{\mathsf T} & E(Z) \end{pmatrix}. \tag*{(11)}

Congruence preserves positive semidefiniteness for either sign of ss. The exact slice (8) gives

Ms(X,Z,y)⪰0⟺Z⪰Φy(X−1),s≠0.(12)M_s(X,Z,y)\succeq0 \quad\Longleftrightarrow\quad Z\succeq\Phi_y(X^{-1}), \qquad s\ne0. \tag*{(12)}

As s→0s\to0, these matrices converge to

M(X,Z,y)=(D(X)B(y)B(y)TE(Z)).M(X,Z,y)=\begin{pmatrix} D(X) & B(y) \\ B(y)^{\mathsf T} & E(Z) \end{pmatrix}.

It follows immediately that Z⪰Φy(X−1)Z\succeq\Phi_y(X^{-1}) implies M(X,Z,y)⪰0M(X,Z,y)\succeq0.

Recovering the inequality from the limit. For the converse, suppose that M(X,Z,y)⪰0M(X,Z,y)\succeq0. Positivity and unitality give

D(X)⪰λmin⁡(X)Ia≻0.D(X)\succeq\lambda_{\min}(X)I_a\succ0.

For every δ>0\delta>0,

M(X,Z+δI4,y)=M(X,Z,y)+diag⁡(0,δIc)≻0.M(X,Z+\delta I_4,y)=M(X,Z,y)+\operatorname{diag}(0,\delta I_c)\succ0.

To see strict positivity, a vector with nonzero lower component has strictly positive contribution from the added term. A nonzero vector with lower component zero has strictly positive quadratic form under D(X)D(X).

Consequently, for each fixed δ>0\delta>0, the matrices Ms(X,Z+δI4,y)M_s(X,Z+\delta I_4,y) are positive definite for sufficiently small nonzero ss. Equation (12) yields Z+δI4⪰Φy(X−1)Z+\delta I_4\succeq\Phi_y(X^{-1}). Letting δ↓0\delta\downarrow0 proves the converse. We have therefore shown

Z⪰Φy(X−1)⟺M(X,Z,y)⪰0.Z\succeq\Phi_y(X^{-1}) \quad\Longleftrightarrow\quad M(X,Z,y)\succeq0.

Taking the Schur complement of the positive definite block D(X)D(X) gives (10).

The maps and their finite dimensions are now fixed by the hypothetical pencil. We next recover the scalar form bb from (10); this will force a nonzero bilinear square dominated by bb and contradict its defining obstruction.

Rank-one limits and a norm identity

Let D,E,BD,E,B be the maps supplied by Proposition 4.1. Thus DD and EE are positive maps with output sizes a,c≥1a,c \ge1 and are unital, meaning D(I4)=IaD(I_4)=I_a and E(I4)=IcE(I_4)=I_c, and B(y)B(y) is an a×ca \times c matrix. For unit vectors u,v∈R4u,v \in\mathbb{R}^4, define the orthogonal projections

P(v)=proj⁡ker⁡D(I−vvT),R(u)=proj⁡ker⁡E(I−uuT).(13)P(v)=\operatorname{proj}_{\ker D(I-vv^{\mathsf T})}, \qquad R(u)=\operatorname{proj}_{\ker E(I-uu^{\mathsf T})}. \tag*{(13)}

These act on Ra\mathbb{R}^a and Rc\mathbb{R}^c, respectively. The next proposition recovers the scalar form (2) from the Schur threshold (10).

Proposition 5.1. Let a,c≥1a,c \ge1, let D:S4→SaD:S^4 \to S^a and E:S4→ScE:S^4 \to S^c be positive unital linear maps, and let B:R3→Ra×cB:\mathbb{R}^3 \to\mathbb{R}^{a\times c} be linear. Assume that (10) holds for every X≻0X \succ0, Z∈S4Z \in S^4 and y∈R3y \in\mathbb{R}^3, with Φy\Phi_y defined by (3). Define P(v)P(v) and R(u)R(u) by (13). For every pair of unit vectors u=(u0,u′)u=(u_0,u'), v=(v0,v′)∈R4v=(v_0,v') \in\mathbb{R}^4 and every y∈R3y \in\mathbb{R}^3,

b(v0u′−u0v′,y)=∥P(v)B(y)R(u)∥op⁡2.(14)b(v_0u'-u_0v',y)=\lVert P(v)B(y)R(u)\rVert_{\operatorname{op}}^2. \tag*{(14)}

Here the operator norm uses the Euclidean structures on the two block spaces.

Proof. Fix u,v,yu,v,y. For t≥1t \ge1, set

Xt=vvT+t(I−vvT),Zt=uuT+t(I−uuT).X_t=vv^{\mathsf T}+t(I-vv^{\mathsf T}), \qquad Z_t=uu^{\mathsf T}+t(I-uu^{\mathsf T}).

Both matrices are at least II. Positivity and unitality therefore give D(Xt)⪰ID(X_t) \succeq I and E(Zt)⪰IE(Z_t) \succeq I, so all inverse square roots below exist. Put

At=Zt−1/2Φy(Xt−1)Zt−1/2,Ct=D(Xt)−1/2B(y)E(Zt)−1/2.A_t=Z_t^{-1/2}\Phi_y(X_t^{-1})Z_t^{-1/2}, \qquad C_t=D(X_t)^{-1/2}B(y)E(Z_t)^{-1/2}.

The matrix AtA_t is positive semidefinite. For every real rr, congruence by Zt−1/2Z_t^{-1/2} gives

rZt⪰Φy(Xt−1)⟺r≥λmax⁡(At).rZ_t \succeq\Phi_y(X_t^{-1}) \quad\Longleftrightarrow\quad r \ge\lambda_{\max}(A_t).

Likewise, linearity of EE and congruence by E(Zt)−1/2E(Z_t)^{-1/2} give

E(rZt)⪰B(y)TD(Xt)−1B(y)⟺rI⪰CtTCt⟺r≥∥Ct∥op⁡2.\begin{aligned} E(rZ_t) &\succeq B(y)^{\mathsf T}D(X_t)^{-1}B(y) \quad\Longleftrightarrow\quad rI \succeq C_t^{\mathsf T}C_t\\ &\Longleftrightarrow\quad r \ge\lVert C_t\rVert_{\operatorname{op}}^2. \end{aligned}

Equation (10) identifies these two closed rays in r∈Rr \in\mathbb{R}, including their endpoints. Consequently,

λmax⁡(At)=∥Ct∥op⁡2.(15)\lambda_{\max}(A_t)=\lVert C_t\rVert_{\operatorname{op}}^2. \tag*{(15)}

This applies to rectangular CtC_t and includes a zero threshold. The explicit formulas

Xt−1=vvT+t−1(I−vvT),Zt−1/2=uuT+t−1/2(I−uuT)X_t^{-1}=vv^{\mathsf T}+t^{-1}(I-vv^{\mathsf T}), \qquad Z_t^{-1/2}=uu^{\mathsf T}+t^{-1/2}(I-uu^{\mathsf T})

show that

At⟶uuTΦy(vvT)uuT=αuuT,α=uTΦy(vvT)u≥0.A_t \longrightarrow uu^{\mathsf T}\Phi_y(vv^{\mathsf T})uu^{\mathsf T}=\alpha uu^{\mathsf T}, \qquad\alpha=u^{\mathsf T}\Phi_y(vv^{\mathsf T})u \ge0.

The sign follows from positivity of Φy\Phi_y. Thus the largest eigenvalue of this limit is α\alpha, also when α=0\alpha=0. Continuity of the largest eigenvalue gives λmax⁡(At)→α\lambda_{\max}(A_t)\to\alpha. For the other side, unitality gives

D(Xt)=I+(t−1)D(I−vvT).D(X_t) = I + (t-1)D(I-vv^{\mathsf T}).

If H⪰0H \succeq0 is a fixed finite-dimensional matrix, diagonalizing HH shows that

[I+(t−1)H]−1/2⟶proj⁡ker⁡H[I+(t-1)H]^{-1/2} \longrightarrow\operatorname{proj}_{\ker H}

in operator norm. {#eq:5.4}

Indeed, the factor on an eigenvector of eigenvalue μ≥0\mu\ge0 is (1+(t−1)μ)−1/2(1+(t-1)\mu)^{-1/2}, which is one when μ=0\mu=0 and tends to zero otherwise. Applying eq:5.4 to D(I−vvT)D(I-vv^{\mathsf T}) and E(I−uuT)E(I-uu^{\mathsf T}) yields

D(Xt)−1/2⟶P(v),E(Zt)−1/2⟶R(u).D(X_t)^{-1/2} \longrightarrow P(v), \qquad E(Z_t)^{-1/2} \longrightarrow R(u).

Hence Ct→P(v)B(y)R(u)C_t \to P(v)B(y)R(u) in operator norm. The dimensions a,ca,c are fixed throughout; the limits include zero and identity kernel projections. Taking limits in (15) and using the rank-one identity (5) proves (14).

At u=vu=v, the left side of (14) vanishes, so P(v)B(y)R(v)=0P(v)B(y)R(v)=0 for every yy. We next study the identity as uu varies near vv.

The tangent obstruction

We finish the proof by taking a first-order limit in the norm identity at a point where the kernel projection varies smoothly. This produces a bilinear matrix whose entries must vanish by Lemma 2.1.

Proof of Theorem 1.1. Proposition 3.1 establishes the polynomial’s degree, normalization, and hyperbolicity. Suppose its closed hyperbolicity cone has a real symmetric pencil representation of some finite size. Fix the maps D,E,BD,E,B supplied by Proposition 4.1, with their fixed finite dimensions a,ca,c. Proposition 5.1 gives (14) for the projections in (13). We shall show that this identity is impossible.

Write S3={u∈R4:∥u∥=1}S^3=\{u\in\mathbb{R}^4:\lVert u\rVert=1\} and consider the symmetric matrix

A(u)=E(I−uuT),u∈Ω:={u∈S3:u0≠0}.A(u)=E(I-uu^{\mathsf T}), \qquad u\in\Omega:=\{u\in S^3:u_0\ne0\}.

Its ranks take only finitely many values, so their maximum ρ\rho is attained at some v∈Ωv\in\Omega. If ρ>0\rho>0, select ρ\rho independent columns of A(v)A(v), and let W(u)W(u) contain the same columns of A(u)A(u). These columns remain independent on a neighborhood of vv in Ω\Omega. By maximality of ρ\rho, they span the range of A(u)A(u) throughout that neighborhood. Symmetry of A(u)A(u) then gives

R(u)=I−W(u)(W(u)TW(u))−1W(u)T.R(u)=I-W(u)\bigl(W(u)^{\mathsf T}W(u)\bigr)^{-1}W(u)^{\mathsf T}.

This is a smooth matrix function. If ρ=0\rho=0, then R(u)=IR(u)=I on Ω\Omega, so it is smooth in this case as well.

Keep vv fixed. At u=vu=v, Equation (14) gives

P(v)B(y)R(v)=0(y∈R3),P(v)B(y)R(v)=0 \qquad(y\in\mathbb{R}^3),

because b(0,y)=0b(0,y)=0. For h=(h0,h′)∈v⊥h=(h_0,h')\in v^\perp, define

Jh=v0h′−h0v′,us=v+sh1+s2∥h∥2.(16)Jh=v_0h'-h_0v', \qquad u_s=\frac{v+sh}{\sqrt{1+s^2\lVert h\rVert^2}}. \tag*{(16)}

For small ss, this path stays in the neighborhood where RR is smooth, and its velocity at zero is hh. Moreover,

v0us′−(us)0v′=sJh1+s2∥h∥2.v_0u_s'-(u_s)_0v'=\frac{sJh}{\sqrt{1+s^2\lVert h\rVert^2}}.

Thus, for s≠0s\ne0, homogeneity of bb and (14) give

b(Jh,y)1+s2∥h∥2=∥P(v)B(y)R(us)−R(v)s∥op2.\frac{b(Jh,y)}{1+s^2\lVert h\rVert^2}=\left\lVert P(v)B(y)\frac{R(u_s)-R(v)}{s}\right\rVert_{\mathrm{op}}^2.

The matrix difference quotient converges to the differential dRv(h)dR_v(h). Passing to the limit by continuity of the operator norm yields

b(Jh,y)=∥P(v)B(y)dRv(h)∥op2(h∈v⊥, y∈R3).(17)b(Jh,y)=\lVert P(v)B(y)dR_v(h)\rVert_{\mathrm{op}}^2\qquad(h\in v^\perp,\ y\in\mathbb{R}^3). \tag*{(17)}

Only RR has been differentiated; the projection P(v)P(v) remains fixed. Figure 1 illustrates this local variation.

Schematic local tangent step showing a local sphere section, $h\perp v$, $\mathbb{S}^3\cap\operatorname{span}\{v,h\}$, and the variation $u_s$; only $R$ is differentiated, $P(v)$ stays fixed

Figure 1. A schematic local tangent step, for a fixed nonzero h∈v⊥h\in v^\perp. The highlighted arc lies in a chosen constant-rank neighborhood UU; the expansion of RR is used only for small ss with us∈Uu_s\in U. The pictured section belongs to the parameter sphere, whereas P(v)P(v) and R(us)R(u_s) act on the separate block spaces Ra\mathbb{R}^a and Rc\mathbb{R}^c.

The linear map J:v⊥→R3J:v^\perp\to\mathbb{R}^3 is an isomorphism. Indeed, if Jh=0Jh=0, then v0≠0v_0\ne0 gives h=(h0/v0)vh=(h_0/v_0)v; since h⊥vh\perp v, this forces h=0h=0. Both spaces have dimension three. Consequently the matrix

F(z,y)=P(v)B(y)dRv(J−1z),z,y∈R3,F(z,y)=P(v)B(y)dR_v(J^{-1}z),\qquad z,y\in\mathbb{R}^3,

has entries that are bilinear in z,yz,y, since BB and the differential dRvdR_v are linear. In fixed orthonormal bases, each entry ℓij(z,y)\ell_{ij}(z,y) satisfies

ℓij(z,y)2≤∥F(z,y)∥op2=b(z,y)(z,y∈R3).\ell_{ij}(z,y)^2\le\lVert F(z,y)\rVert_{\mathrm{op}}^2=b(z,y)\qquad(z,y\in\mathbb{R}^3).

Lemma 2.1 forces every entry to vanish identically. Equation (6.1) would therefore make bb identically zero, contradicting b(e1,e1)=1b(e_1,e_1)=1. This excludes the hypothetical finite pencil and completes the proof.

Removing a determinant factor

The polynomial pp makes the positive-map construction explicit through a 4×44\times4 determinant. We now remove a factor that is unnecessary for its hyperbolicity cone. A larger block determinant shows directly that the quotient remains polynomial at singular XX.

Proof of Corollary 1.2. For the standard coordinate vectors eie_i of R3\mathbb{R}^3, put

Ki=(0eiT−ei0)∈R4×4,C=(K1K2K3)∈R4×12.K_i=\begin{pmatrix}0&e_i^{\mathsf{T}}\\-e_i&0\end{pmatrix}\in\mathbb{R}^{4\times4},\qquad C=\begin{pmatrix}K_1&K_2&K_3\end{pmatrix}\in\mathbb{R}^{4\times12}.

Here U⊗VU\otimes V denotes the block matrix with blocks UijVU_{ij}V. Direct block multiplication in (3) gives, for T∈S4T\in\mathbb{S}^4,

Φy(T)=∑i,j=13Q(y)ijKiTKjT=C(Q(y)⊗T)CT.\Phi_y(T)=\sum_{i,j=1}^{3}Q(y)_{ij}K_iTK_j^{\mathsf{T}}=C\bigl(Q(y)\otimes T\bigr)C^{\mathsf{T}}.

Define the polynomial

q(X,Z,y)=det⁡(I3⊗XCTC(Q(y)⊗I4)Z).(18)q(X,Z,y)=\det\begin{pmatrix}I_3\otimes X&C^{\mathsf{T}}\\C\bigl(Q(y)\otimes I_4\bigr)&Z\end{pmatrix}. \tag*{(18)}

For invertible XX, taking a Schur complement yields

q(X,Z,y)=(det⁡X)3det⁡(Z−Φy(X−1)).q(X,Z,y)=(\det X)^3\det\bigl(Z-\Phi_y(X^{-1})\bigr).

Comparison with (7) proves the polynomial identity

p(X,Z,y)=(det⁡X)q(X,Z,y)(19)p(X,Z,y)=(\det X)q(X,Z,y) \tag*{(19)}

first for invertible XX and then everywhere by continuity. Since pp and det⁡X\det X are homogeneous of degrees 20 and 4, this identity makes qq homogeneous of degree 16; also q(e)=1q(e)=1. For each real (X,Z,y)(X,Z,y), the polynomial q(te−(X,Z,y))q(te-(X,Z,y)) is a factor of the real-rooted polynomial p(te−(X,Z,y))p(te-(X,Z,y)). Hence qq is hyperbolic with respect to ee.

Write Kq=Λ+(q,e)K_q=\Lambda_+(q,e). The factorization (19) gives

K={(X,Z,y):X⪰0}∩Kq,(20)K=\{(X,Z,y):X\succeq0\}\cap K_q, \tag*{(20)}

because the roots contributed by det⁡(tI4−X)\det(tI_4-X) are the eigenvalues of XX. It remains to show that KqK_q already forces X⪰0X\succeq0. The polynomial qq is even in yy, so (X,Z,y)∈Kq(X,Z,y)\in K_q implies (X,Z,−y)∈Kq(X,Z,-y)\in K_q. By convexity of hyperbolicity cones [6], their midpoint (X,Z,0)(X,Z,0) also belongs to KqK_q. But eq:7.1 gives

q(X,Z,0)=(det⁡X)3det⁡Z,q(X,Z,0)=(\det X)^3\det Z,

whose closed hyperbolicity cone in this slice is exactly {(X,Z,0):X⪰0, Z⪰0}\{(X,Z,0):X\succeq0,\ Z\succeq0\}. Thus X⪰0X\succeq0 throughout KqK_q, and (20) implies Kq=KK_q=K. Theorem 1.1 now supplies nonspectrahedrality.

A path-containment assertion

Theorem 53 (pp. 16–17) of version 1 of González Nevado’s [7] states a positive solution of the geometric Generalized Lax conjecture. Its proof invokes Theorem 52 (p. 16), which asserts containment of a fixed rigidly convex set throughout a smooth real-zero deformation from a product of normalized tangent linear factors to a multiple of the defining polynomial. The following example violates that intermediate assertion under its stated hypotheses.

A real polynomial gg with g(0)=1g(0)=1 is real-zero if the roots of s↦g(sx)s\mapsto g(sx) are real for every real vector xx. Its closed rigidly convex set is the closure of the component of {g≠0}\{g\ne0\} containing the origin. Fix a,b,η>0a,b,\eta>0 and, in one variable, put

g(x)=(1−x/a)(1+x/b),c(t)=1+ηsin⁡2(πt),Ht(x)=g(c(t)x),0≤t≤1.g(x)=(1-x/a)(1+x/b),\qquad c(t)=1+\eta\sin^2(\pi t),\qquad H_t(x)=g(c(t)x),\qquad0\le t\le1.

The zero set of gg is the compact smooth set {−b,a}\{-b,a\}. The normalized tangent linear factors at these two points are 1+x/b1+x/b and 1−x/a1-x/a, whose product is gg. Every HtH_t has value 11 at the origin and two distinct real roots,

−bc(t)andac(t).-\frac{b}{c(t)} \quad\text{and}\quad\frac{a}{c(t)}.

Thus the path depends smoothly on tt and consists of real-zero polynomials with compact smooth zero sets. It even admits the smooth monic real symmetric determinantal representation

Ht(x)=det⁡(1−c(t)x/a001+c(t)x/b).H_t(x)=\det\begin{pmatrix}1-c(t)x/a & 0 \\ 0 & 1+c(t)x/b\end{pmatrix}.

Both endpoints equal gg, so the final polynomial is gg times the constant cofactor 11, as allowed by the stated hypotheses. Nevertheless the rigidly convex set of HtH_t is

[−bc(t),ac(t)],\left[-\frac{b}{c(t)},\frac{a}{c(t)}\right],

which is strictly smaller than [−b,a][-b,a] whenever 0<t<10<t<1. Consequently it does not contain the rigidly convex set of gg.

The parameters a,b>0a,b>0 describe the open family of normalized real quadratics with negative leading coefficient, so the failure is not confined to a symmetric or multiple-root example. The parameter η\eta may be arbitrarily small. The cited Theorem 52 states no restriction to two or more variables, no lower bound on pencil size, and no requirement that the endpoint cofactor be nonconstant.

This example refutes the all-intermediate-times conclusion of that theorem. Its endpoints coincide, so it does not refute an endpoint-only statement. The nonspectrahedrality result of this paper follows from the construction and obstruction proved above.

References

  1. [1]Grigoriy Blekherman, Bogdan Raiță, Isabelle Shankar, and Rainer Sinn. Weak and strong extremal biquadratics, 2022. URL https://arxiv.org/abs/2204.10625v1. Version 1.
  2. [2]Petter Brändén. Obstructions to determinantal representability. Advances in Mathematics, 226(2):1202–1212, 2011. doi: 10.1016/j.aim.2010.08.003. URL https://arxiv.org/abs/1004.1382.
  3. [3]Man-Duen Choi. Positive semidefinite biquadratic forms. Linear Algebra and its Applications, 12(2):95–100, 1975. doi: 10.1016/0024-3795(75)90058-0.DOI
  4. [4]Man-Duen Choi and Tsit-Yuen Lam. Extremal positive semidefinite forms. Mathematische Annalen, 231(1):1–18, 1977. doi: 10.1007/BF01360024.DOI
  5. [5]Papri Dey, Stephan Gardoll, and Thorsten Theobald. Conic stability of polynomials and positive maps. Journal of Pure and Applied Algebra, 225(7):106610, 2021. doi: 10.1016/j.jpaa.2020.106610. URL https://arxiv.org/abs/1908.11124v2.
  6. [6]Lars Gårding. An inequality for hyperbolic polynomials. Journal of Mathematics and Mechanics, 8(6):957–965, 1959. doi: 10.1512/iumj.1959.8.58061. URL https://doi.org/10.1512/iumj.1959.8.58061.
  7. [7]Alejandro González Nevado. The generalized Lax conjecture is true for topological reasons related to compactness, convexity and determinantal deformations of increasing products of pointwise approximating linear forms, 2026. URL https://arxiv.org/abs/2601.12267v1. Version 1, 18 January 2026.
  8. [8]Kil-Chan Ha. Notes on extremality of the Choi map. Linear Algebra and its Applications, 439 (10):3156–3165, 2013. doi: 10.1016/j.laa.2013.09.011. URL https://arxiv.org/abs/1306.0945v1.
  9. [9]J. William Helton and Victor Vinnikov. Linear matrix inequality representation of sets. Communications on Pure and Applied Mathematics, 60(5):654–674, 2007. doi: 10.1002/cpa.20155. URL https://arxiv.org/abs/math/0306180.
  10. [10]Mario Kummer. A note on the hyperbolicity cone of the specialized Vámos polynomial. Acta Applicandae Mathematicae, 144(1):11–15, 2016. doi: 10.1007/s10440-015-0036-z. URL https://arxiv.org/abs/1306.4483.
  11. [11]Mario Kummer and Tim Netzer. The generalized Lax conjecture for strictly hyperbolic polynomials, 2026. URL https://arxiv.org/abs/2609.24542v1. Version 1, 21 September 2026.
  12. [12]Peter D. Lax. Differential equations, difference equations and matrix theory. Communications on Pure and Applied Mathematics, 11(2):175–194, 1958. doi: 10.1002/cpa.3160110203.DOI
  13. [13]Adrian S. Lewis, Pablo A. Parrilo, and Motakuri V. Ramana. The Lax conjecture is true. Proceedings of the American Mathematical Society, 133(9):2495–2499, 2005. doi: 10.1090/S0002-9939-05-07752-X. URL https://arxiv.org/abs/math/0304104.
  14. [14]Tim Netzer. Clifford realizations of hyperbolic cubics, 2026. URL https://arxiv.org/abs/2609.12957v1. Version 1, 11 September 2026.
  15. [15]Tim Netzer and Raman Sanyal. Smooth hyperbolicity cones are spectrahedral shadows. Mathematical Programming, 153:213–221, 2015. doi: 10.1007/s10107-014-0744-6. URL https://arxiv.org/abs/1208.0441.
  16. [16]Prasad Raghavendra, Nick Ryder, Nikhil Srivastava, and Benjamin Weitz. Exponential lower bounds on spectrahedral representations of hyperbolicity cones. In Timothy M. Chan, editor, Proceedings of the Thirtieth Annual ACM–SIAM Symposium on Discrete Algorithms, pages 2322–2332. Society for Industrial and Applied Mathematics, 2019. doi: 10.1137/1.9781611975482.141. URL https://arxiv.org/abs/1711.11497v2.
  17. [17]Claus Scheiderer. Spectrahedral shadows. SIAM Journal on Applied Algebra and Geometry, 2(1):26–44, 2018. doi: 10.1137/17M1118981. URL https://epubs.siam.org/doi/pdf/10.1137/17M1118981.DOI

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