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 |
---|---|---|---|---|---|---|---|---|---|
1540 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{6}\phi_{1}^{2}$ | 0.6559 | 0.8059 | 0.8139 | [M:[1.0498, 0.7503, 0.9502, 0.8498, 1.1502, 1.1], q:[0.5751, 0.3752], qb:[0.4747, 0.775], phi:[0.45]] | [M:[[22], [-30], [-22], [14], [-14], [4]], q:[[-7], [-15]], qb:[[29], [1]], phi:[[-2]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
---|---|---|---|---|
${}M_{2}$, ${ }M_{4}$, ${ }M_{3}$, ${ }M_{1}$, ${ }M_{6}$, ${ }M_{5}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{4}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{4}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}M_{3}$, ${ }M_{1}M_{2}$, ${ }M_{3}M_{4}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{2}M_{6}$, ${ }M_{3}^{2}$, ${ }M_{2}M_{5}$, ${ }M_{4}M_{6}$, ${ }M_{2}\phi_{1}q_{2}^{2}$ | ${}$ | -1 | t^2.251 + t^2.55 + t^2.851 + t^3.149 + t^3.3 + t^3.45 + t^3.601 + t^3.9 + t^4.05 + t^4.198 + t^4.201 + t^4.499 + t^4.502 + 2*t^4.801 + t^5.099 + t^5.102 + t^5.4 + t^5.551 + t^5.701 + t^5.849 + t^5.852 - t^6. + 2*t^6.151 + t^6.301 + 2*t^6.449 + 2*t^6.452 + t^6.748 + 2*t^6.75 + t^6.753 + t^6.901 + t^7.049 + 3*t^7.052 + t^7.202 + t^7.347 + 2*t^7.35 + t^7.353 + 2*t^7.501 + t^7.649 + 2*t^7.651 + t^7.799 + 2*t^7.802 + t^7.952 + t^8.098 + 2*t^8.1 + t^8.103 - t^8.251 + t^8.396 + t^8.399 + 3*t^8.402 - 2*t^8.55 + t^8.552 + t^8.697 + 2*t^8.7 + 2*t^8.703 - t^8.848 - 2*t^8.851 + 2*t^8.999 - t^4.35/y - t^6.601/y + t^7.801/y + t^8.099/y + t^8.102/y + (2*t^8.4)/y + t^8.551/y + t^8.699/y + t^8.701/y + t^8.849/y - t^4.35*y - t^6.601*y + t^7.801*y + t^8.099*y + t^8.102*y + 2*t^8.4*y + t^8.551*y + t^8.699*y + t^8.701*y + t^8.849*y | t^2.251/g1^30 + g1^14*t^2.55 + t^2.851/g1^22 + g1^22*t^3.149 + g1^4*t^3.3 + t^3.45/g1^14 + t^3.601/g1^32 + g1^12*t^3.9 + t^4.05/g1^6 + g1^56*t^4.198 + t^4.201/g1^24 + g1^20*t^4.499 + t^4.502/g1^60 + (2*t^4.801)/g1^16 + g1^28*t^5.099 + t^5.102/g1^52 + t^5.4/g1^8 + t^5.551/g1^26 + t^5.701/g1^44 + g1^18*t^5.849 + t^5.852/g1^62 - t^6. + (2*t^6.151)/g1^18 + t^6.301/g1^36 + 2*g1^26*t^6.449 + (2*t^6.452)/g1^54 + g1^70*t^6.748 + (2*t^6.75)/g1^10 + t^6.753/g1^90 + t^6.901/g1^28 + g1^34*t^7.049 + (3*t^7.052)/g1^46 + t^7.202/g1^64 + g1^78*t^7.347 + (2*t^7.35)/g1^2 + t^7.353/g1^82 + (2*t^7.501)/g1^20 + g1^42*t^7.649 + (2*t^7.651)/g1^38 + g1^24*t^7.799 + (2*t^7.802)/g1^56 + t^7.952/g1^74 + g1^68*t^8.098 + (2*t^8.1)/g1^12 + t^8.103/g1^92 - t^8.251/g1^30 + g1^112*t^8.396 + g1^32*t^8.399 + (3*t^8.402)/g1^48 - 2*g1^14*t^8.55 + t^8.552/g1^66 + g1^76*t^8.697 + (2*t^8.7)/g1^4 + (2*t^8.703)/g1^84 - g1^58*t^8.848 - (2*t^8.851)/g1^22 + 2*g1^40*t^8.999 - t^4.35/(g1^2*y) - t^6.601/(g1^32*y) + t^7.801/(g1^16*y) + (g1^28*t^8.099)/y + t^8.102/(g1^52*y) + (2*t^8.4)/(g1^8*y) + t^8.551/(g1^26*y) + (g1^36*t^8.699)/y + t^8.701/(g1^44*y) + (g1^18*t^8.849)/y - (t^4.35*y)/g1^2 - (t^6.601*y)/g1^32 + (t^7.801*y)/g1^16 + g1^28*t^8.099*y + (t^8.102*y)/g1^52 + (2*t^8.4*y)/g1^8 + (t^8.551*y)/g1^26 + g1^36*t^8.699*y + (t^8.701*y)/g1^44 + g1^18*t^8.849*y |
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 |
---|---|---|---|---|---|---|---|---|---|
983 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{1}M_{3}$ | 0.6651 | 0.8215 | 0.8096 | [M:[1.0528, 0.7461, 0.9472, 0.8518, 1.1482], q:[0.5741, 0.3731], qb:[0.4788, 0.7751], phi:[0.4497]] | t^2.238 + t^2.555 + t^2.698 + t^2.841 + t^3.159 + t^3.445 + t^3.588 + t^3.905 + t^4.048 + t^4.191 + t^4.222 + t^4.477 + t^4.508 + 2*t^4.794 + t^4.937 + t^5.08 + t^5.111 + t^5.254 + 2*t^5.397 + t^5.54 + t^5.683 + t^5.826 + t^5.857 - t^6. - t^4.349/y - t^4.349*y | detail |