6,152 research outputs found

    Graphs with small diameter determined by their DD-spectra

    Get PDF
    Let GG be a connected graph with vertex set V(G)={v1,v2,...,vn}V(G)=\{v_{1},v_{2},...,v_{n}\}. The distance matrix D(G)=(dij)n×nD(G)=(d_{ij})_{n\times n} is the matrix indexed by the vertices of G,G, where dijd_{ij} denotes the distance between the vertices viv_{i} and vjv_{j}. Suppose that λ1(D)≥λ2(D)≥⋯≥λn(D)\lambda_{1}(D)\geq\lambda_{2}(D)\geq\cdots\geq\lambda_{n}(D) are the distance spectrum of GG. The graph GG is said to be determined by its DD-spectrum if with respect to the distance matrix D(G)D(G), any graph having the same spectrum as GG is isomorphic to GG. In this paper, we give the distance characteristic polynomial of some graphs with small diameter, and also prove that these graphs are determined by their DD-spectra

    Constraints on the Asymptotic Baryon Fractions of Galaxy Clusters at Large Radii

    Get PDF
    While X-ray measurements have so far revealed an increase in the volume-averaged baryon fractions fb(r)f_b(r) of galaxy clusters with cluster radii rr, fb(r)f_b(r) should asymptotically reach a universal value fb(∞)=fbf_b(\infty)=f_b, provided that clusters are representative of the Universe. In the framework of hydrostatic equilibrium for intracluster gas, we have derived the necessary conditions for fb(∞)=fbf_b(\infty)=f_b: The X-ray surface brightness profile described by the β\beta model and the temperature profile approximated by the polytropic model should satisfy γ≈2(1−1/3β)\gamma\approx2(1-1/3\beta) and γ≈1+1/3β\gamma\approx1+1/3\beta for β1\beta1, respectively, which sets a stringent limit to the polytropic index: γ<4/3\gamma<4/3. In particular, a mildly increasing temperature with radius is required if the observationally fitted β\beta parameter is in the range 1/3<β<2/31/3<\beta<2/3. It is likely that a reliable determination of the universal baryon fraction can be achieved in the small β\beta clusters because the disagreement between the exact and asymptotic baryon fractions for clusters with β>2/3\beta>2/3 breaks down at rather large radii (\ga30r_c) where hydrostatic equilibrium has probably become inapplicable. We further explore how to obtain the asymptotic value fb(∞)f_b(\infty) of baryon fraction from the X-ray measurement made primarily over the finite central region of a cluster. We demonstrate our method using a sample of 19 strong lensing clusters, which enables us to place a useful constraint on fb(∞)f_b(\infty): 0.094±0.035≤fb(∞)≤0.41±0.180.094\pm0.035 \leq f_b(\infty) \leq 0.41\pm0.18. An optimal estimate of fb(∞)f_b(\infty) based on three cooling flow clusters with β=0.142±0.007\beta = 0.142\pm0.007 or ΩM=0.35±0.09\Omega_M = 0.35\pm0.09.Comment: 6 pages + 4 figures; accepted for publication in MNRA
    • …
    corecore