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![Figure 1: Sequential growth rule: displayed is one branch point of Tand one inner edge only; the three associated possibilities forattached to it; all edges also carry weights, weight 1n with degree k + 1, hencevertex weight (k − 1)α − γ, with k − r leaves Lr+1,..., Lk ∈ [n] and r bigger subtrees S1,...,Sr − α and γ are displayed here for one leaf edge Tn+1 are displayed.](https://thumb-ap.123doks.com/thumbv2/123dok/983483.916661/5.612.92.507.91.250/sequential-displayed-associated-possibilities-forattached-hencevertex-displayed-displayed.webp)
![Figure 2: We display an example ofdashed lines, white leaves) and further subtrees in the branch points of S(T16,[3]), seven skeletal subtrees in five skeletal bushes (within the S(T16,[3]) (with black leaves).](https://thumb-ap.123doks.com/thumbv2/123dok/983483.916661/27.612.216.380.86.265/figure-display-example-ofdashed-subtrees-skeletal-subtrees-skeletal.webp)
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In this paper, it is shown that each starlike tree with maximum degree 4 is determined by its signless Laplacian spectrum..
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Tajbakhsh and Omidi showed that starlike trees are determined by their Laplacian spectra (see [6]). In this paper, we show that each starlike tree with maximum degree 4 is determined
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Although it can be reduced to Kempf’s commutation relation by applying some transformations to the position and momentum operators, we have shown that it gives rise to more
