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 |
---|---|---|---|---|---|---|---|---|---|
4077 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{5}\phi_{1}q_{2}^{2}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ + ${ }M_{5}M_{6}$ + ${ }M_{7}q_{1}q_{2}$ + ${ }M_{4}M_{8}$ | 0.6633 | 0.8079 | 0.821 | [M:[0.9977, 1.1259, 0.9359, 0.6888, 0.7506, 1.2494, 0.8124, 1.3112], q:[0.7815, 0.4062], qb:[0.5961, 0.468], phi:[0.4371]] | [M:[[32], [-12], [22], [-18], [-8], [8], [2], [18]], q:[[-3], [1]], qb:[[-33], [11]], phi:[[6]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
---|---|---|---|---|
${}M_{7}$, ${ }\phi_{1}^{2}$, ${ }M_{3}$, ${ }M_{1}$, ${ }M_{2}$, ${ }M_{6}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{8}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{7}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }M_{3}M_{7}$, ${ }\phi_{1}^{4}$, ${ }M_{1}M_{7}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{3}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{1}^{2}$ | ${}$ | -2 | t^2.437 + t^2.622 + t^2.808 + t^2.993 + t^3.378 + 2*t^3.748 + t^3.934 + t^4.119 + t^4.133 + t^4.318 + t^4.503 + t^4.874 + t^4.888 + t^5.059 + 2*t^5.245 + t^5.43 + t^5.615 + t^5.801 + t^5.986 - 2*t^6. + t^6.185 + 3*t^6.371 - t^6.385 + 3*t^6.556 + 3*t^6.741 + t^6.755 + t^6.927 + t^6.941 + t^7.112 + t^7.126 + t^7.311 + t^7.325 + 3*t^7.497 + t^7.51 + 3*t^7.682 + 4*t^7.867 + t^7.881 + 2*t^8.053 + t^8.066 + 2*t^8.238 + t^8.252 + t^8.266 + 2*t^8.423 - 3*t^8.437 + t^8.609 - t^8.622 + 2*t^8.636 + t^8.794 - 2*t^8.808 - t^8.822 + t^8.979 + t^8.993 - t^4.311/y - t^6.748/y - t^7.119/y - t^7.304/y + t^7.318/y + t^7.503/y + t^7.874/y + t^8.059/y + t^8.245/y + (2*t^8.43)/y + t^8.615/y + t^8.801/y + t^8.815/y - t^4.311*y - t^6.748*y - t^7.119*y - t^7.304*y + t^7.318*y + t^7.503*y + t^7.874*y + t^8.059*y + t^8.245*y + 2*t^8.43*y + t^8.615*y + t^8.801*y + t^8.815*y | g1^2*t^2.437 + g1^12*t^2.622 + g1^22*t^2.808 + g1^32*t^2.993 + t^3.378/g1^12 + 2*g1^8*t^3.748 + g1^18*t^3.934 + g1^28*t^4.119 + t^4.133/g1^36 + t^4.318/g1^26 + t^4.503/g1^16 + g1^4*t^4.874 + t^4.888/g1^60 + g1^14*t^5.059 + 2*g1^24*t^5.245 + g1^34*t^5.43 + g1^44*t^5.615 + g1^54*t^5.801 + g1^64*t^5.986 - 2*t^6. + g1^10*t^6.185 + 3*g1^20*t^6.371 - t^6.385/g1^44 + 3*g1^30*t^6.556 + 3*g1^40*t^6.741 + t^6.755/g1^24 + g1^50*t^6.927 + t^6.941/g1^14 + g1^60*t^7.112 + t^7.126/g1^4 + g1^6*t^7.311 + t^7.325/g1^58 + 3*g1^16*t^7.497 + t^7.51/g1^48 + 3*g1^26*t^7.682 + 4*g1^36*t^7.867 + t^7.881/g1^28 + 2*g1^46*t^8.053 + t^8.066/g1^18 + 2*g1^56*t^8.238 + t^8.252/g1^8 + t^8.266/g1^72 + 2*g1^66*t^8.423 - 3*g1^2*t^8.437 + g1^76*t^8.609 - g1^12*t^8.622 + (2*t^8.636)/g1^52 + g1^86*t^8.794 - 2*g1^22*t^8.808 - t^8.822/g1^42 + g1^96*t^8.979 + g1^32*t^8.993 - (g1^6*t^4.311)/y - (g1^8*t^6.748)/y - (g1^28*t^7.119)/y - (g1^38*t^7.304)/y + t^7.318/(g1^26*y) + t^7.503/(g1^16*y) + (g1^4*t^7.874)/y + (g1^14*t^8.059)/y + (g1^24*t^8.245)/y + (2*g1^34*t^8.43)/y + (g1^44*t^8.615)/y + (g1^54*t^8.801)/y + t^8.815/(g1^10*y) - g1^6*t^4.311*y - g1^8*t^6.748*y - g1^28*t^7.119*y - g1^38*t^7.304*y + (t^7.318*y)/g1^26 + (t^7.503*y)/g1^16 + g1^4*t^7.874*y + g1^14*t^8.059*y + g1^24*t^8.245*y + 2*g1^34*t^8.43*y + g1^44*t^8.615*y + g1^54*t^8.801*y + (t^8.815*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 |
---|
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 |
---|
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 |
---|
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 |
---|---|---|---|---|---|---|---|---|---|
1690 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{5}\phi_{1}q_{2}^{2}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ + ${ }M_{5}M_{6}$ + ${ }M_{7}q_{1}q_{2}$ | 0.684 | 0.8481 | 0.8065 | [M:[1.0011, 1.1246, 0.9383, 0.6869, 0.7497, 1.2503, 0.8126], q:[0.7811, 0.4063], qb:[0.5926, 0.4691], phi:[0.4377]] | t^2.061 + t^2.438 + t^2.626 + t^2.815 + t^3.003 + t^3.374 + 2*t^3.751 + 2*t^4.121 + t^4.128 + t^4.31 + 2*t^4.498 + t^4.687 + t^4.869 + 2*t^4.875 + 2*t^5.064 + 2*t^5.253 + t^5.434 + t^5.441 + t^5.63 + 2*t^5.811 + t^5.818 - 2*t^6. - t^4.313/y - t^4.313*y | detail | {a: 137580491/201130032, c: 85290089/100565016, M1: 6148/6141, M2: 2302/2047, M3: 5762/6141, M4: 1406/2047, M5: 4604/6141, M6: 7678/6141, M7: 4990/6141, q1: 1599/2047, q2: 2495/6141, qb1: 1213/2047, qb2: 2881/6141, phi1: 896/2047} |