Chosen Fixed Point
Here is the data for the chosen fixed point.
$F_{UV}$ represents the flavor symmetries in the UV Lagrangian, and $F_{IR}$ represents the flavor symmetries in the IR. $F_{UV}$ and $F_{IR}$ can differ due to accidental symmetry enhancement.
The number of marginal operators, $n_{marginal}$, minus the dimension of flavor symmetries in IR, $|F_{IR}|$, corresponds to the coefficient of $t^6$ in the superconformal index.
# | Theory | Superpotential | Central charge $a$ | Central charge $c$ | Ratio $a/c$ | Matter field: $R$-charge | U(1) part of $F_{UV}$ | Rank of $F_{UV}$ | Rational |
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57048 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{4}\phi_{1}q_{2}^{2}$ + ${ }M_{1}M_{4}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ + ${ }M_{6}\phi_{1}^{2}$ + ${ }M_{7}\phi_{1}q_{1}q_{2}$ | 0.6679 | 0.8375 | 0.7975 | [M:[1.1174, 0.7277, 0.8826, 0.8826, 0.6761, 1.2207, 0.7277], q:[0.5188, 0.3639], qb:[0.7535, 0.8052], phi:[0.3897]] | [M:[[-16], [-14], [16], [16], [-24], [4], [-14]], q:[[23], [-7]], qb:[[-9], [1]], phi:[[-2]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{5}$, ${ }M_{2}$, ${ }M_{7}$, ${ }M_{3}$, ${ }M_{4}$, ${ }M_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{6}$, ${ }M_{5}^{2}$, ${ }M_{2}M_{5}$, ${ }M_{5}M_{7}$, ${ }\phi_{1}q_{1}^{2}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{7}$, ${ }M_{7}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{3}M_{5}$, ${ }M_{4}M_{5}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}M_{3}$, ${ }M_{2}M_{4}$, ${ }M_{3}M_{7}$, ${ }M_{4}M_{7}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{4}^{2}$, ${ }M_{1}M_{5}$, ${ }M_{1}M_{2}$, ${ }M_{1}M_{7}$, ${ }M_{5}q_{2}\tilde{q}_{2}$, ${ }M_{5}M_{6}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{2}q_{2}\tilde{q}_{2}$, ${ }M_{7}q_{2}\tilde{q}_{2}$, ${ }M_{2}M_{6}$, ${ }M_{6}M_{7}$ | ${}$ | -2 | t^2.028 + 2*t^2.183 + 2*t^2.648 + t^3.352 + t^3.507 + t^3.662 + t^4.056 + 2*t^4.211 + t^4.282 + 3*t^4.366 + t^4.521 + 3*t^4.676 + 3*t^4.831 + t^4.986 + 2*t^5.296 + t^5.38 + 2*t^5.535 + 4*t^5.69 + t^5.845 - 2*t^6. + t^6.085 + t^6.155 + 2*t^6.24 + 2*t^6.31 + 3*t^6.394 + 5*t^6.549 + 4*t^6.704 + 5*t^6.859 + 2*t^6.929 + 5*t^7.014 + t^7.169 + 2*t^7.324 + t^7.409 + 2*t^7.479 + 2*t^7.563 + 5*t^7.718 + 6*t^7.873 + 2*t^7.944 + t^8.113 - 4*t^8.183 + 2*t^8.268 + 3*t^8.338 + 3*t^8.423 - t^8.493 + t^8.563 + 5*t^8.578 - 5*t^8.648 + 9*t^8.732 + 6*t^8.887 + 2*t^8.958 - t^4.169/y - t^6.197/y - (2*t^6.352)/y - t^6.817/y + (2*t^7.211)/y + t^7.366/y + t^7.521/y + (2*t^7.676)/y + (4*t^7.831)/y + (2*t^7.986)/y + t^8.141/y - t^8.225/y + t^8.296/y - t^8.38/y + (3*t^8.69)/y + t^8.845/y - t^4.169*y - t^6.197*y - 2*t^6.352*y - t^6.817*y + 2*t^7.211*y + t^7.366*y + t^7.521*y + 2*t^7.676*y + 4*t^7.831*y + 2*t^7.986*y + t^8.141*y - t^8.225*y + t^8.296*y - t^8.38*y + 3*t^8.69*y + t^8.845*y | t^2.028/g1^24 + (2*t^2.183)/g1^14 + 2*g1^16*t^2.648 + t^3.352/g1^16 + t^3.507/g1^6 + g1^4*t^3.662 + t^4.056/g1^48 + (2*t^4.211)/g1^38 + g1^44*t^4.282 + (3*t^4.366)/g1^28 + t^4.521/g1^18 + (3*t^4.676)/g1^8 + 3*g1^2*t^4.831 + g1^12*t^4.986 + 2*g1^32*t^5.296 + t^5.38/g1^40 + (2*t^5.535)/g1^30 + (4*t^5.69)/g1^20 + t^5.845/g1^10 - 2*t^6. + t^6.085/g1^72 + g1^10*t^6.155 + (2*t^6.24)/g1^62 + 2*g1^20*t^6.31 + (3*t^6.394)/g1^52 + (5*t^6.549)/g1^42 + (4*t^6.704)/g1^32 + (5*t^6.859)/g1^22 + 2*g1^60*t^6.929 + (5*t^7.014)/g1^12 + t^7.169/g1^2 + 2*g1^8*t^7.324 + t^7.409/g1^64 + 2*g1^18*t^7.479 + (2*t^7.563)/g1^54 + (5*t^7.718)/g1^44 + (6*t^7.873)/g1^34 + 2*g1^48*t^7.944 + t^8.113/g1^96 - (4*t^8.183)/g1^14 + (2*t^8.268)/g1^86 + (3*t^8.338)/g1^4 + (3*t^8.423)/g1^76 - g1^6*t^8.493 + g1^88*t^8.563 + (5*t^8.578)/g1^66 - 5*g1^16*t^8.648 + (9*t^8.732)/g1^56 + (6*t^8.887)/g1^46 + 2*g1^36*t^8.958 - t^4.169/(g1^2*y) - t^6.197/(g1^26*y) - (2*t^6.352)/(g1^16*y) - (g1^14*t^6.817)/y + (2*t^7.211)/(g1^38*y) + t^7.366/(g1^28*y) + t^7.521/(g1^18*y) + (2*t^7.676)/(g1^8*y) + (4*g1^2*t^7.831)/y + (2*g1^12*t^7.986)/y + (g1^22*t^8.141)/y - t^8.225/(g1^50*y) + (g1^32*t^8.296)/y - t^8.38/(g1^40*y) + (3*t^8.69)/(g1^20*y) + t^8.845/(g1^10*y) - (t^4.169*y)/g1^2 - (t^6.197*y)/g1^26 - (2*t^6.352*y)/g1^16 - g1^14*t^6.817*y + (2*t^7.211*y)/g1^38 + (t^7.366*y)/g1^28 + (t^7.521*y)/g1^18 + (2*t^7.676*y)/g1^8 + 4*g1^2*t^7.831*y + 2*g1^12*t^7.986*y + g1^22*t^8.141*y - (t^8.225*y)/g1^50 + g1^32*t^8.296*y - (t^8.38*y)/g1^40 + (3*t^8.69*y)/g1^20 + (t^8.845*y)/g1^10 |
Deformation
Here is the data for the deformed fixed points from the chosen fixed point.
# | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
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Equivalent Fixed Points from Other Seed Theories
Here is a list of equivalent fixed points from other gauge theories.
# | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
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Equivalent Fixed Points from the Same Seed Theory
Below is a list of equivalent fixed points from the same seed theories.
id | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | More Info. | Rational |
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Previous Theory
The previous fixed point before deforming to get the chosen fixed point.
# | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
---|---|---|---|---|---|---|---|---|---|
55478 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{4}\phi_{1}q_{2}^{2}$ + ${ }M_{1}M_{4}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ + ${ }M_{6}\phi_{1}^{2}$ | 0.6481 | 0.8005 | 0.8096 | [M:[1.122, 0.7318, 0.878, 0.878, 0.6831, 1.2195], q:[0.5121, 0.3659], qb:[0.7562, 0.8049], phi:[0.3903]] | t^2.049 + t^2.195 + 2*t^2.634 + t^3.366 + t^3.512 + t^3.658 + t^3.805 + t^4.098 + t^4.243 + t^4.245 + t^4.391 + t^4.537 + 3*t^4.683 + t^4.829 + t^4.975 + 2*t^5.268 + t^5.415 + t^5.562 + 3*t^5.708 + t^5.854 - t^6. - t^4.171/y - t^4.171*y | detail |