Landscape




$a$ =

$c$ =

$\leq a \leq$

$\leq c \leq$

id =





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.

#TheorySuperpotentialCentral charge $a$Central charge $c$Ratio $a/c$Matter field: $R$-chargeU(1) part of $F_{UV}$Rank of $F_{UV}$Rational
3035 SU2adj1nf2 ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{1}M_{4}$ + ${ }M_{5}\phi_{1}^{2}$ + ${ }M_{6}q_{1}q_{2}$ + ${ }M_{7}q_{1}\tilde{q}_{1}$ 0.6628 0.8259 0.8025 [M:[1.1264, 0.7356, 0.8736, 0.8736, 1.2184, 0.6897, 0.8276], q:[0.8046, 0.5057], qb:[0.3678, 0.7586], phi:[0.3908]] [M:[[16], [14], [-16], [-16], [-4], [24], [-6]], q:[[-1], [-23]], qb:[[7], [9]], phi:[[2]]] 1 {a: 26755/40368, c: 16669/20184, M1: 98/87, M2: 64/87, M3: 76/87, M4: 76/87, M5: 106/87, M6: 20/29, M7: 24/29, q1: 70/87, q2: 44/87, qb1: 32/87, qb2: 22/29, phi1: 34/87}
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
${}M_{6}$, ${ }M_{2}$, ${ }M_{7}$, ${ }M_{3}$, ${ }M_{4}$, ${ }M_{1}$, ${ }M_{5}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{6}^{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{2}M_{6}$, ${ }M_{2}^{2}$, ${ }M_{6}M_{7}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}M_{6}$, ${ }M_{4}M_{6}$, ${ }M_{2}M_{7}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{2}M_{3}$, ${ }M_{2}M_{4}$, ${ }M_{7}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{3}M_{7}$, ${ }M_{4}M_{7}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{4}^{2}$, ${ }M_{1}M_{6}$, ${ }M_{5}M_{6}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{2}M_{5}$, ${ }M_{1}M_{7}$, ${ }M_{6}\phi_{1}q_{2}\tilde{q}_{1}$ ${}$ -1 t^2.069 + t^2.207 + t^2.483 + 2*t^2.621 + t^3.379 + t^3.655 + t^3.793 + t^4.138 + t^4.207 + t^4.276 + t^4.414 + 2*t^4.552 + 4*t^4.69 + t^4.828 + 2*t^4.966 + 2*t^5.103 + 2*t^5.241 + t^5.448 + 2*t^5.724 + 2*t^5.862 - t^6. + t^6.207 + 3*t^6.276 + t^6.345 + t^6.414 + t^6.483 + 3*t^6.621 + t^6.69 + 4*t^6.759 + 2*t^6.828 + 2*t^6.897 + 3*t^7.034 + 4*t^7.172 + 3*t^7.31 + 3*t^7.448 + t^7.517 + 3*t^7.586 + t^7.724 + 2*t^7.793 + 2*t^7.862 + 3*t^7.931 + t^8. - t^8.069 - 2*t^8.207 + t^8.276 + 4*t^8.345 + 2*t^8.414 - 2*t^8.483 + t^8.552 - 4*t^8.621 + 3*t^8.69 + 2*t^8.759 + 5*t^8.828 + 3*t^8.897 + 2*t^8.966 - t^4.172/y - t^6.241/y - t^6.379/y - t^6.655/y - t^6.793/y + t^7.276/y + (2*t^7.552)/y + (4*t^7.69)/y + (2*t^7.828)/y + t^7.966/y + (3*t^8.103)/y + t^8.241/y - t^8.31/y + t^8.862/y - t^4.172*y - t^6.241*y - t^6.379*y - t^6.655*y - t^6.793*y + t^7.276*y + 2*t^7.552*y + 4*t^7.69*y + 2*t^7.828*y + t^7.966*y + 3*t^8.103*y + t^8.241*y - t^8.31*y + t^8.862*y g1^24*t^2.069 + g1^14*t^2.207 + t^2.483/g1^6 + (2*t^2.621)/g1^16 + g1^16*t^3.379 + t^3.655/g1^4 + t^3.793/g1^14 + g1^48*t^4.138 + t^4.207/g1^44 + g1^38*t^4.276 + g1^28*t^4.414 + 2*g1^18*t^4.552 + 4*g1^8*t^4.69 + t^4.828/g1^2 + (2*t^4.966)/g1^12 + (2*t^5.103)/g1^22 + (2*t^5.241)/g1^32 + g1^40*t^5.448 + 2*g1^20*t^5.724 + 2*g1^10*t^5.862 - t^6. + g1^72*t^6.207 + (3*t^6.276)/g1^20 + g1^62*t^6.345 + t^6.414/g1^30 + g1^52*t^6.483 + 3*g1^42*t^6.621 + t^6.69/g1^50 + 4*g1^32*t^6.759 + (2*t^6.828)/g1^60 + 2*g1^22*t^6.897 + 3*g1^12*t^7.034 + 4*g1^2*t^7.172 + (3*t^7.31)/g1^8 + (3*t^7.448)/g1^18 + g1^64*t^7.517 + (3*t^7.586)/g1^28 + t^7.724/g1^38 + 2*g1^44*t^7.793 + (2*t^7.862)/g1^48 + 3*g1^34*t^7.931 + t^8./g1^58 - g1^24*t^8.069 - 2*g1^14*t^8.207 + g1^96*t^8.276 + 4*g1^4*t^8.345 + t^8.414/g1^88 + g1^86*t^8.414 - (2*t^8.483)/g1^6 + g1^76*t^8.552 - (4*t^8.621)/g1^16 + 3*g1^66*t^8.69 + (2*t^8.759)/g1^26 + 5*g1^56*t^8.828 + (3*t^8.897)/g1^36 + 2*g1^46*t^8.966 - (g1^2*t^4.172)/y - (g1^26*t^6.241)/y - (g1^16*t^6.379)/y - t^6.655/(g1^4*y) - t^6.793/(g1^14*y) + (g1^38*t^7.276)/y + (2*g1^18*t^7.552)/y + (4*g1^8*t^7.69)/y + (2*t^7.828)/(g1^2*y) + t^7.966/(g1^12*y) + (3*t^8.103)/(g1^22*y) + t^8.241/(g1^32*y) - (g1^50*t^8.31)/y + (g1^10*t^8.862)/y - g1^2*t^4.172*y - g1^26*t^6.241*y - g1^16*t^6.379*y - (t^6.655*y)/g1^4 - (t^6.793*y)/g1^14 + g1^38*t^7.276*y + 2*g1^18*t^7.552*y + 4*g1^8*t^7.69*y + (2*t^7.828*y)/g1^2 + (t^7.966*y)/g1^12 + (3*t^8.103*y)/g1^22 + (t^8.241*y)/g1^32 - g1^50*t^8.31*y + g1^10*t^8.862*y


Deformation

Here is the data for the deformed fixed points from the chosen fixed point.

#SuperpotentialCentral Charge $a$ Central Charge $c$ Ratio $a/c$$R$-chargesSuperconformal IndexMore Info.Rational


Equivalent Fixed Points from Other Seed Theories

Here is a list of equivalent fixed points from other gauge theories.

#TheorySuperpotentialCentral Charge $a$ Central Charge $c$ Ratio $a/c$$R$-chargesSuperconformal IndexMore 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.

#TheorySuperpotentialCentral Charge $a$ Central Charge $c$ Ratio $a/c$$R$-chargesSuperconformal IndexMore Info.Rational
1982 SU2adj1nf2 ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{1}M_{4}$ + ${ }M_{5}\phi_{1}^{2}$ + ${ }M_{6}q_{1}q_{2}$ 0.6481 0.8005 0.8096 [M:[1.122, 0.7318, 0.878, 0.878, 1.2195, 0.6831], q:[0.8049, 0.5121], qb:[0.3659, 0.7562], 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