gp: [N,k,chi] = [1027,4,Mod(1,1027)]
mf = mfinit([N,k,chi],0)
lf = mfeigenbasis(mf)
magma: // Please install CHIMP (https://github.com/edgarcosta/CHIMP) if you want to run this code
chi := DirichletCharacter("1027.1");
S:= CuspForms(chi, 4);
N := Newforms(S);
sage: from sage.modular.dirichlet import DirichletCharacter
H = DirichletGroup(1027, base_ring=CyclotomicField(2))
chi = DirichletCharacter(H, H._module([0, 0]))
N = Newforms(chi, 4, names="a")
Newform invariants
sage: traces = [56,-16]
f = next(g for g in N if [g.coefficient(i+1).trace() for i in range(2)] == traces)
gp: f = lf[1] \\ Warning: the index may be different
The algebraic \(q\)-expansion of this newform has not been computed, but we have computed the trace expansion .
For each embedding \(\iota_m\) of the coefficient field, the values \(\iota_m(a_n)\) are shown below.
For more information on an embedded modular form you can click on its label.
gp: mfembed(f)
Refresh table
\( p \)
Sign
\(13\)
\( +1 \)
\(79\)
\( -1 \)
This newform does not admit any (nontrivial ) inner twists .
This newform subspace can be constructed as the kernel of the linear operator
\( T_{2}^{56} + 16 T_{2}^{55} - 200 T_{2}^{54} - 4428 T_{2}^{53} + 13526 T_{2}^{52} + 568899 T_{2}^{51} + \cdots + 49\!\cdots\!76 \)
T2^56 + 16*T2^55 - 200*T2^54 - 4428*T2^53 + 13526*T2^52 + 568899*T2^51 + 143257*T2^50 - 45008595*T2^49 - 93309374*T2^48 + 2451299559*T2^47 + 8243393322*T2^46 - 97245948708*T2^45 - 435018878690*T2^44 + 2895570546764*T2^43 + 16256948251089*T2^42 - 65510300485242*T2^41 - 458875771124369*T2^40 + 1119742165368870*T2^39 + 10110372772228794*T2^38 - 13934505600211623*T2^37 - 177212509807126517*T2^36 + 110078197412980609*T2^35 + 2499096387720255951*T2^34 - 140524654534104019*T2^33 - 28536865546804219984*T2^32 - 10834026053285057349*T2^31 + 264611088077610624454*T2^30 + 191668468178153075390*T2^29 - 1992650999290843695700*T2^28 - 1995851605166604947382*T2^27 + 12159187792990411844579*T2^26 + 14913734266096523449308*T2^25 - 59862331516475156145350*T2^24 - 84297426533999728883488*T2^23 + 236308271996174787282206*T2^22 + 366404024149716128448985*T2^21 - 742062813615445459090939*T2^20 - 1226080953784136631719482*T2^19 + 1836543983615732343600260*T2^18 + 3132066849418918632769316*T2^17 - 3546354226182496996630348*T2^16 - 6005395520466389056210776*T2^15 + 5289469519210122926357856*T2^14 + 8412455694861582076798624*T2^13 - 6033255615217196280105216*T2^12 - 8257532810823765708851584*T2^11 + 5188672922336354082885376*T2^10 + 5308427861382408152502272*T2^9 - 3252459169020098218156032*T2^8 - 1971818965709723809370112*T2^7 + 1362925654159152156041216*T2^6 + 302788632004055291731968*T2^5 - 315730552967398811385856*T2^4 + 16712006551030107996160*T2^3 + 27498567216435026264064*T2^2 - 6877316883774398791680*T2 + 491218196375818469376
acting on \(S_{4}^{\mathrm{new}}(\Gamma_0(1027))\).